HEPData Search

Table 1

Ratio of deuterons to protons for polar angle 20-30 deg.

Table 2

Ratio of deuterons to protons for polar angle 30-45 deg.

Table 3

Ratio of deuterons to protons for polar angle 45-65 deg.

Table 4

Ratio of deuterons to protons for polar angle 65-90 deg.

Table 5

Ratio of deuterons to protons for polar angle 90-125 deg.

Table 6

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in P Tin interactions at a beam energy of 3 GeV.

Table 7

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in P Tin interactions at a beam energy of 3 GeV.

Table 8

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in P Tin interactions at a beam energy of 3 GeV.

Table 9

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in P Tin interactions at a beam energy of 3 GeV.

Table 10

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in P Tin interactions at a beam energy of 3 GeV.

Table 11

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in P Tin interactions at a beam energy of 3 GeV.

Table 12

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in P Tin interactions at a beam energy of 3 GeV.

Table 13

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in P Tin interactions at a beam energy of 3 GeV.

Table 14

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 3 GeV.

Table 15

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 3 GeV.

Table 16

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 3 GeV.

Table 17

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 3 GeV.

Table 18

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 3 GeV.

Table 19

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 3 GeV.

Table 20

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 3 GeV.

Table 21

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 3 GeV.

Table 22

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI- Tin interactions at a beam energy of 3 GeV.

Table 23

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI- Tin interactions at a beam energy of 3 GeV.

Table 24

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI- Tin interactions at a beam energy of 3 GeV.

Table 25

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI- Tin interactions at a beam energy of 3 GeV.

Table 26

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI- Tin interactions at a beam energy of 3 GeV.

Table 27

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI- Tin interactions at a beam energy of 3 GeV.

Table 28

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI- Tin interactions at a beam energy of 3 GeV.

Table 29

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI- Tin interactions at a beam energy of 3 GeV.

Table 30

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 3 GeV.

Table 31

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 3 GeV.

Table 32

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 3 GeV.

Table 33

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 3 GeV.

Table 34

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 3 GeV.

Table 35

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 3 GeV.

Table 36

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 3 GeV.

Table 37

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 3 GeV.

Table 38

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 3 GeV.

Table 39

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 3 GeV.

Table 40

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 3 GeV.

Table 41

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 3 GeV.

Table 42

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 3 GeV.

Table 43

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 3 GeV.

Table 44

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 3 GeV.

Table 45

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 3 GeV.

Table 46

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 3 GeV.

Table 47

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 3 GeV.

Table 48

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 3 GeV.

Table 49

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 3 GeV.

Table 50

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 3 GeV.

Table 51

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 3 GeV.

Table 52

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 3 GeV.

Table 53

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 3 GeV.

Table 54

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in P Tin interactions at a beam energy of 3 GeV.

Table 55

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in P Tin interactions at a beam energy of 3 GeV.

Table 56

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in P Tin interactions at a beam energy of 3 GeV.

Table 57

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in P Tin interactions at a beam energy of 3 GeV.

Table 58

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in P Tin interactions at a beam energy of 3 GeV.

Table 59

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in P Tin interactions at a beam energy of 3 GeV.

Table 60

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in P Tin interactions at a beam energy of 3 GeV.

Table 61

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in P Tin interactions at a beam energy of 3 GeV.

Table 62

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 3 GeV.

Table 63

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 3 GeV.

Table 64

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 3 GeV.

Table 65

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 3 GeV.

Table 66

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 3 GeV.

Table 67

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 3 GeV.

Table 68

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 3 GeV.

Table 69

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 3 GeV.

Table 70

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 3 GeV.

Table 71

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 3 GeV.

Table 72

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 3 GeV.

Table 73

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 3 GeV.

Table 74

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 3 GeV.

Table 75

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 3 GeV.

Table 76

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 3 GeV.

Table 77

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 3 GeV.

Table 78

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in P Tin interactions at a beam energy of 5 GeV.

Table 79

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in P Tin interactions at a beam energy of 5 GeV.

Table 80

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in P Tin interactions at a beam energy of 5 GeV.

Table 81

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in P Tin interactions at a beam energy of 5 GeV.

Table 82

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in P Tin interactions at a beam energy of 5 GeV.

Table 83

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in P Tin interactions at a beam energy of 5 GeV.

Table 84

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in P Tin interactions at a beam energy of 5 GeV.

Table 85

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in P Tin interactions at a beam energy of 5 GeV.

Table 86

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 5 GeV.

Table 87

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 5 GeV.

Table 88

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 5 GeV.

Table 89

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 5 GeV.

Table 90

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 5 GeV.

Table 91

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 5 GeV.

Table 92

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 5 GeV.

Table 93

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 5 GeV.

Table 94

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI- Tin interactions at a beam energy of 5 GeV.

Table 95

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI- Tin interactions at a beam energy of 5 GeV.

Table 96

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI- Tin interactions at a beam energy of 5 GeV.

Table 97

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI- Tin interactions at a beam energy of 5 GeV.

Table 98

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI- Tin interactions at a beam energy of 5 GeV.

Table 99

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI- Tin interactions at a beam energy of 5 GeV.

Table 100

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI- Tin interactions at a beam energy of 5 GeV.

Table 101

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI- Tin interactions at a beam energy of 5 GeV.

Table 102

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 5 GeV.

Table 103

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 5 GeV.

Table 104

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 5 GeV.

Table 105

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 5 GeV.

Table 106

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 5 GeV.

Table 107

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 5 GeV.

Table 108

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 5 GeV.

Table 109

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 5 GeV.

Table 110

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 5 GeV.

Table 111

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 5 GeV.

Table 112

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 5 GeV.

Table 113

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 5 GeV.

Table 114

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 5 GeV.

Table 115

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 5 GeV.

Table 116

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 5 GeV.

Table 117

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 5 GeV.

Table 118

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 5 GeV.

Table 119

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 5 GeV.

Table 120

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 5 GeV.

Table 121

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 5 GeV.

Table 122

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 5 GeV.

Table 123

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 5 GeV.

Table 124

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 5 GeV.

Table 125

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 5 GeV.

Table 126

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in P Tin interactions at a beam energy of 5 GeV.

Table 127

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in P Tin interactions at a beam energy of 5 GeV.

Table 128

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in P Tin interactions at a beam energy of 5 GeV.

Table 129

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in P Tin interactions at a beam energy of 5 GeV.

Table 130

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in P Tin interactions at a beam energy of 5 GeV.

Table 131

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in P Tin interactions at a beam energy of 5 GeV.

Table 132

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in P Tin interactions at a beam energy of 5 GeV.

Table 133

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in P Tin interactions at a beam energy of 5 GeV.

Table 134

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 5 GeV.

Table 135

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 5 GeV.

Table 136

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 5 GeV.

Table 137

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 5 GeV.

Table 138

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 5 GeV.

Table 139

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 5 GeV.

Table 140

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 5 GeV.

Table 141

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 5 GeV.

Table 142

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 5 GeV.

Table 143

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 5 GeV.

Table 144

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 5 GeV.

Table 145

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 5 GeV.

Table 146

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 5 GeV.

Table 147

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 5 GeV.

Table 148

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 5 GeV.

Table 149

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 5 GeV.

Table 150

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in P Tin interactions at a beam energy of 8 GeV.

Table 151

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in P Tin interactions at a beam energy of 8 GeV.

Table 152

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in P Tin interactions at a beam energy of 8 GeV.

Table 153

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in P Tin interactions at a beam energy of 8 GeV.

Table 154

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in P Tin interactions at a beam energy of 8 GeV.

Table 155

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in P Tin interactions at a beam energy of 8 GeV.

Table 156

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in P Tin interactions at a beam energy of 8 GeV.

Table 157

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in P Tin interactions at a beam energy of 8 GeV.

Table 158

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 8 GeV.

Table 159

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 8 GeV.

Table 160

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 8 GeV.

Table 161

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 8 GeV.

Table 162

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 8 GeV.

Table 163

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 8 GeV.

Table 164

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 8 GeV.

Table 165

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 8 GeV.

Table 166

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI- Tin interactions at a beam energy of 8 GeV.

Table 167

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI- Tin interactions at a beam energy of 8 GeV.

Table 168

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI- Tin interactions at a beam energy of 8 GeV.

Table 169

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI- Tin interactions at a beam energy of 8 GeV.

Table 170

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI- Tin interactions at a beam energy of 8 GeV.

Table 171

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI- Tin interactions at a beam energy of 8 GeV.

Table 172

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI- Tin interactions at a beam energy of 8 GeV.

Table 173

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI- Tin interactions at a beam energy of 8 GeV.

Table 174

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 8 GeV.

Table 175

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 8 GeV.

Table 176

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 8 GeV.

Table 177

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 8 GeV.

Table 178

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 8 GeV.

Table 179

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 8 GeV.

Table 180

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 8 GeV.

Table 181

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 8 GeV.

Table 182

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 8 GeV.

Table 183

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 8 GeV.

Table 184

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 8 GeV.

Table 185

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 8 GeV.

Table 186

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 8 GeV.

Table 187

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 8 GeV.

Table 188

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 8 GeV.

Table 189

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 8 GeV.

Table 190

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 8 GeV.

Table 191

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 8 GeV.

Table 192

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 8 GeV.

Table 193

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 8 GeV.

Table 194

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 8 GeV.

Table 195

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 8 GeV.

Table 196

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 8 GeV.

Table 197

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 8 GeV.

Table 198

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in P Tin interactions at a beam energy of 8 GeV.

Table 199

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in P Tin interactions at a beam energy of 8 GeV.

Table 200

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in P Tin interactions at a beam energy of 8 GeV.

Table 201

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in P Tin interactions at a beam energy of 8 GeV.

Table 202

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in P Tin interactions at a beam energy of 8 GeV.

Table 203

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in P Tin interactions at a beam energy of 8 GeV.

Table 204

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in P Tin interactions at a beam energy of 8 GeV.

Table 205

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in P Tin interactions at a beam energy of 8 GeV.

Table 206

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 8 GeV.

Table 207

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 8 GeV.

Table 208

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 8 GeV.

Table 209

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 8 GeV.

Table 210

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 8 GeV.

Table 211

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 8 GeV.

Table 212

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 8 GeV.

Table 213

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 8 GeV.

Table 214

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 8 GeV.

Table 215

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 8 GeV.

Table 216

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 8 GeV.

Table 217

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 8 GeV.

Table 218

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 8 GeV.

Table 219

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 8 GeV.

Table 220

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 8 GeV.

Table 221

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 8 GeV.

Table 222

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in P Tin interactions at a beam energy of 12 GeV.

Table 223

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in P Tin interactions at a beam energy of 12 GeV.

Table 224

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in P Tin interactions at a beam energy of 12 GeV.

Table 225

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in P Tin interactions at a beam energy of 12 GeV.

Table 226

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in P Tin interactions at a beam energy of 12 GeV.

Table 227

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in P Tin interactions at a beam energy of 12 GeV.

Table 228

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in P Tin interactions at a beam energy of 12 GeV.

Table 229

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in P Tin interactions at a beam energy of 12 GeV.

Table 230

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 12 GeV.

Table 231

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 12 GeV.

Table 232

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 12 GeV.

Table 233

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 12 GeV.

Table 234

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 12 GeV.

Table 235

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 12 GeV.

Table 236

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 12 GeV.

Table 237

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 12 GeV.

Table 238

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI- Tin interactions at a beam energy of 12 GeV.

Table 239

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI- Tin interactions at a beam energy of 12 GeV.

Table 240

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI- Tin interactions at a beam energy of 12 GeV.

Table 241

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI- Tin interactions at a beam energy of 12 GeV.

Table 242

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI- Tin interactions at a beam energy of 12 GeV.

Table 243

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI- Tin interactions at a beam energy of 12 GeV.

Table 244

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI- Tin interactions at a beam energy of 12 GeV.

Table 245

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI- Tin interactions at a beam energy of 12 GeV.

Table 246

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 12 GeV.

Table 247

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 12 GeV.

Table 248

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 12 GeV.

Table 249

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 12 GeV.

Table 250

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 12 GeV.

Table 251

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 12 GeV.

Table 252

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 12 GeV.

Table 253

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 12 GeV.

Table 254

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 12 GeV.

Table 255

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 12 GeV.

Table 256

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 12 GeV.

Table 257

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 12 GeV.

Table 258

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 12 GeV.

Table 259

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 12 GeV.

Table 260

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 12 GeV.

Table 261

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 12 GeV.

Table 262

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 12 GeV.

Table 263

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 12 GeV.

Table 264

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 12 GeV.

Table 265

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 12 GeV.

Table 266

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 12 GeV.

Table 267

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 12 GeV.

Table 268

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 12 GeV.

Table 269

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 12 GeV.

Table 270

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in P Tin interactions at a beam energy of 12 GeV.

Table 271

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in P Tin interactions at a beam energy of 12 GeV.

Table 272

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in P Tin interactions at a beam energy of 12 GeV.

Table 273

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in P Tin interactions at a beam energy of 12 GeV.

Table 274

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in P Tin interactions at a beam energy of 12 GeV.

Table 275

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in P Tin interactions at a beam energy of 12 GeV.

Table 276

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in P Tin interactions at a beam energy of 12 GeV.

Table 277

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in P Tin interactions at a beam energy of 12 GeV.

Table 278

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 12 GeV.

Table 279

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 12 GeV.

Table 280

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 12 GeV.

Table 281

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 12 GeV.

Table 282

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 12 GeV.

Table 283

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 12 GeV.

Table 284

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 12 GeV.

Table 285

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 12 GeV.

Table 286

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 12 GeV.

Table 287

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 12 GeV.

Table 288

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 12 GeV.

Table 289

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 12 GeV.

Table 290

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 12 GeV.

Table 291

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 12 GeV.

Table 292

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 12 GeV.

Table 293

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 12 GeV.

Table 294

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in P Tin interactions at a beam energy of 15 GeV.

Table 295

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in P Tin interactions at a beam energy of 15 GeV.

Table 296

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in P Tin interactions at a beam energy of 15 GeV.

Table 297

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in P Tin interactions at a beam energy of 15 GeV.

Table 298

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in P Tin interactions at a beam energy of 15 GeV.

Table 299

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in P Tin interactions at a beam energy of 15 GeV.

Table 300

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in P Tin interactions at a beam energy of 15 GeV.

Table 301

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in P Tin interactions at a beam energy of 15 GeV.

Table 302

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 15 GeV.

Table 303

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 15 GeV.

Table 304

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 15 GeV.

Table 305

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 15 GeV.

Table 306

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 15 GeV.

Table 307

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 15 GeV.

Table 308

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 15 GeV.

Table 309

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 15 GeV.

Table 310

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI- Tin interactions at a beam energy of 15 GeV.

Table 311

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI- Tin interactions at a beam energy of 15 GeV.

Table 312

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI- Tin interactions at a beam energy of 15 GeV.

Table 313

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI- Tin interactions at a beam energy of 15 GeV.

Table 314

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI- Tin interactions at a beam energy of 15 GeV.

Table 315

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI- Tin interactions at a beam energy of 15 GeV.

Table 316

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI- Tin interactions at a beam energy of 15 GeV.

Table 317

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI- Tin interactions at a beam energy of 15 GeV.

Table 318

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 15 GeV.

Table 319

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 15 GeV.

Table 320

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 15 GeV.

Table 321

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 15 GeV.

Table 322

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 15 GeV.

Table 323

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 15 GeV.

Table 324

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 15 GeV.

Table 325

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 15 GeV.

Table 326

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 15 GeV.

Table 327

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 15 GeV.

Table 328

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 15 GeV.

Table 329

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 15 GeV.

Table 330

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 15 GeV.

Table 331

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 15 GeV.

Table 332

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 15 GeV.

Table 333

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 15 GeV.

Table 334

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 15 GeV.

Table 335

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 15 GeV.

Table 336

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 15 GeV.

Table 337

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 15 GeV.

Table 338

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 15 GeV.

Table 339

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 15 GeV.

Table 340

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 15 GeV.

Table 341

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 15 GeV.

Table 342

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in P Tin interactions at a beam energy of 15 GeV.

Table 343

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in P Tin interactions at a beam energy of 15 GeV.

Table 344

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in P Tin interactions at a beam energy of 15 GeV.

Table 345

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in P Tin interactions at a beam energy of 15 GeV.

Table 346

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in P Tin interactions at a beam energy of 15 GeV.

Table 347

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in P Tin interactions at a beam energy of 15 GeV.

Table 348

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in P Tin interactions at a beam energy of 15 GeV.

Table 349

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in P Tin interactions at a beam energy of 15 GeV.

Table 350

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 15 GeV.

Table 351

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 15 GeV.

Table 352

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 15 GeV.

Table 353

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 15 GeV.

Table 354

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 15 GeV.

Table 355

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 15 GeV.

Table 356

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 15 GeV.

Table 357

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 15 GeV.

Table 358

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 15 GeV.

Table 359

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 15 GeV.

Table 360

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 15 GeV.

Table 361

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 15 GeV.

Table 362

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 15 GeV.

Table 363

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 15 GeV.

Table 364

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 15 GeV.

Table 365

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 15 GeV.

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Cross-sections of large-angle hadron production in proton- and pion-nucleus interactions VII: tin nuclei and beam momenta from \pm3 GeV/c to \pm15 GeV/c

NEUTRON TO PROTON RATIOS IN p A AND pi+- A INTERACTIONS