A Measurement of the Nucleon Structure Function From Muon Carbon Deep Inelastic Scattering at High $Q^2$

The BCDMS collaboration Bollini, D. ; Frabetti, P.L. ; Heiman, G. ; et al.
Phys.Lett. B104 (1981) 403-408, 1981.
Inspire Record 166160 DOI 10.17182/hepdata.71276
8 data tables

No description provided.

No description provided.

No description provided.

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Nuclear structure function in carbon near x = 1

The BCDMS collaboration Benvenuti, A.C. ; Bollini, D. ; Camporesi, T. ; et al.
Z.Phys. C63 (1994) 29-36, 1994.
Inspire Record 374300 DOI 10.17182/hepdata.48235
5 data tables

No description provided.

Multiplicative factors by which F2 has to be multiplied or divided to allow for a systematic uncertainty in detector resolution.

Multiplicative factors by which F2 has to be multiplied or divided to allow for a systematic uncertainty in the beam energy.

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A Comparison of the Structure Functions F2 of the Proton and the Neutron From Deep Inelastic Muon Scattering at High $Q^2$

The BCDMS collaboration Benvenuti, A.C. ; Bollini, D. ; Bruni, G. ; et al.
Phys.Lett. B237 (1990) 599-604, 1990.
Inspire Record 285519 DOI 10.17182/hepdata.29734
2 data tables

No description provided.

No description provided.


A High Statistics Measurement of the Deuteron Structure Functions F2 (X, $Q^2$) and R From Deep Inelastic Muon Scattering at High $Q^2$

The BCDMS collaboration Benvenuti, A.C. ; Bollini, D. ; Bruni, G. ; et al.
Phys.Lett. B237 (1990) 592-598, 1990.
Inspire Record 285497 DOI 10.17182/hepdata.6191
87 data tables

No description provided.

R=SIG(L)/SIG(T) is taken to be zero.

R=SIG(L)/SIG(T) is taken to be zero.

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NEW RESULTS ON NUCLEAR EFFECTS IN DEEP INELASTIC MUON SCATTERING ON DEUTERIUM AND IRON TARGETS

The BCDMS collaboration Benvenuti, A.C. ; Bollini, D. ; Bruni, G. ; et al.
Conference Paper, 1986.
Inspire Record 238756 DOI 10.17182/hepdata.39470
2 data tables

VALUES OBTAINED USING ASSUMPTION R=0.

VALUES OBTAINED USING ASSUMPTION R=0.


Nuclear Effects in Deep Inelastic Muon Scattering on Deuterium and Iron Targets

The BCDMS collaboration Benvenuti, A.C. ; Bollini, D. ; Bruni, G. ; et al.
Phys.Lett. B189 (1987) 483-487, 1987.
Inspire Record 244886 DOI 10.17182/hepdata.30200
1 data table

Q**2 RANGE FOR EACH X BIN IS AS FOLLOWS: 14 TO 20, 16 TO 30, 18 TO 35, 18 TO 46, 20 TO 106, 23 TO 106, 23 TO 150, 26 TO 200, 26 TO 200, 26 TO 200 GEV**2.


A High Statistics Measurement of the Nucleon Structure Function F(2) (X,$Q^2$) From Deep Inelastic Muon - Carbon Scattering at High $Q^2$

The BCDMS collaboration Benvenuti, A.C. ; Bollini, D. ; Bruni, G. ; et al.
Phys.Lett. B195 (1987) 91-96, 1987.
Inspire Record 247013 DOI 10.17182/hepdata.30107
19 data tables

R=SIG(L)/SIG(T).

No description provided.

No description provided.

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A High Statistics Measurement of the Proton Structure Functions F(2) (x, Q**2) and R from Deep Inelastic Muon Scattering at High Q**2

The BCDMS collaboration Benvenuti, A.C. ; Bollini, D. ; Bruni, G. ; et al.
Phys.Lett. B223 (1989) 485-489, 1989.
Inspire Record 276661 DOI 10.17182/hepdata.12557
105 data tables

THE AVERAGE VALUES OF Q**2 AT EACH OF THE X VALUES LISTED IN THIS TABLE ARE 15,20,20,25,30,35,40,45,50,50.

R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.

R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.

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A Measurement of Nuclear Effects in Deep Inelastic Muon Scattering on Deuterium, Nitrogen and Iron Targets

The BCDMS collaboration Bari, G. ; Benvenuti, A.C. ; Bollini, D. ; et al.
Phys.Lett. B163 (1985) 282, 1985.
Inspire Record 216817 DOI 10.17182/hepdata.30331
2 data tables

VALUES OF Q2 CORRESPONDING TO THE X-BINS IN THIS TABLE ARE:- 46-106,46-106,53-150,53-200,70-200,80-200 RESPECTIVELY.

VALUES OF Q2 CORRESPONDING TO THE X-BINS IN THIS TABLE ARE:- 26-40,26-61,30-80,30-106,30-106,30-150,30-200,35-200,46-200.