The A dependence of the nuclear structure function ratios

The New Muon collaboration Arneodo, M. ; Arvidson, A. ; Badelek, B. ; et al.
Nucl.Phys. B481 (1996) 3-22, 1996.
Inspire Record 429851 DOI 10.17182/hepdata.32712
6 data tables

Additional normalisation error of 0.002 in the ratio.

Additional normalisation error of 0.002 in the ratio.

Additional normalisation error of 0.003 in the ratio.

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The Q**2 dependence of the structure function ratio F2 Sn / F2 C and the difference R Sn - R C in deep inelastic muon scattering

The New Muon collaboration Arneodo, M. ; Arvidson, A. ; Badelek, B. ; et al.
Nucl.Phys. B481 (1996) 23-39, 1996.
Inspire Record 429850 DOI 10.17182/hepdata.32717
17 data tables

Additional normalisation error in the ratio of 0.002.

Additional normalisation error in the ratio of 0.002.

Additional normalisation error in the ratio of 0.002.

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Shadowing in inelastic scattering of muons on carbon, calcium and lead at low x(Bj)

The E665 collaboration Adams, M.R. ; Aid, S. ; Anthony, P.L. ; et al.
Z.Phys. C67 (1995) 403-410, 1995.
Inspire Record 394981 DOI 10.17182/hepdata.41664

Nuclear shadowing is observed in the per-nucleon cross-sections of positive muons on carbon, calcium and lead as compared to deuterium. The data were taken by Fermilab experiment E665 using inelastically scattered muons of mean incident momentum 470 GeV/c. Cross-section ratios are presented in the kinematic region 0.0001 < XBj <0.56 and 0.1 < Q**2 < 80 GeVc. The data are consistent with no significant nu or Q**2 dependence at fixed XBj. As XBj decreases, the size of the shadowing effect, as well as its A dependence, are found to approach the corresponding measurements in photoproduction.

4 data tables

Per-nucleon cross section ratio for carbon to deuterium.

Per-nucleon cross section ratio for calcium to deuterium.

Per-nucleon cross section ratio for lead to deuterium.

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A Reevaluation of the nuclear structure function ratios for D, He, Li-6, C and Ca

The New Muon collaboration Amaudruz, P. ; Arneodo, M. ; Arvidson, A. ; et al.
Nucl.Phys. B441 (1995) 3-11, 1995.
Inspire Record 393377 DOI 10.17182/hepdata.32848

We present a re-evaluation of the structure function ratios F2(He)/F2(D), F2(C)/F2(D) and F2(Ca)/F2(D) measured in deep inelastic muon-nucleus scattering at an incident muon momentum of 200 GeV. We also present the ratios F2(C)/F2(Li), F2(Ca)/F2(Li) and F2(Ca)/F2(C) measured at 90 GeV. The results are based on data already published by NMC; the main difference in the analysis is a correction for the masses of the deuterium targets and an improvement in the radiative corrections. The kinematic range covered is 0.0035 < x < 0.65, 0.5 < Q~2 <90 GeV~2 for the He/D, C/D and Ca/D data and 0.0085 < x < 0.6, 0.84 < Q~2 < 17 GeV~2 for the Li/C/Ca ones.

6 data tables

Additional normalization uncertainty of 0.4 pct not included.

Additional normalization uncertainty of 0.4 pct not included.

Additional normalization uncertainty of 0.4 pct not included.

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The Structure Function ratios F2(li) / F2(D) and F2(C) / F2(D) at small x

The New Muon collaboration Arneodo, M. ; Arvidson, A. ; Badelek, B. ; et al.
Nucl.Phys. B441 (1995) 12-30, 1995.
Inspire Record 394050 DOI 10.17182/hepdata.47955

We present the structure function ratios F2(Li)/F2(D) and F2(C)/F2(D) measured in deep inelastic muon-nucleus scattering at a nominal incident muon energy of 200 GeV. The kinematic range 0.0001 < x < 0.7 and 0.01< Q~2 < 70 GeV~2 is covered. For values of $x$ less than $0.002$ both ratios indicate saturation of shadowing at values compatible with photoabsorption results.

2 data tables

Additional normalization error of 0.004 not included.

Data on F2(C)/F2(DEUT) merged with previous NMC data from Amaudruz et al. 1995, NP B441,3. (<a href=http://durpdg.dur.ac.uk/scripts/reacsearch.csh/TESTREAC/red+3106> RED = 3106 </a>). Additional normalization error of 0.004 not included.


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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Saturation of shadowing at very low $x_{\rm BJ}$

The E665 collaboration Adams, M.R. ; Aid, S. ; Anthony, P.L. ; et al.
Phys.Rev.Lett. 68 (1992) 3266-3269, 1992.
Inspire Record 333894 DOI 10.17182/hepdata.19864
2 data tables

Data using Electromagnetic Cuts.

Data using Hadron Requirement.


Shadowing in the muon xenon inelastic scattering cross-section at 490-GeV

The Fermilab E665 collaboration Adams, M.R. ; Aid, S. ; Anthony, P.L. ; et al.
Phys.Lett. B287 (1992) 375-380, 1992.
Inspire Record 341389 DOI 10.17182/hepdata.29153
2 data tables

Xenon structure function parameterized as being equal to the DEUT structurefunction.

Xenon structure function parameterized by an x-dependent shadowing factor times the DEUT structure function.


A Measurement of the ratio of the nucleon structure function in copper and deuterium

The European Muon collaboration Ashman, J. ; Badelek, B. ; Baum, Guenter ; et al.
Z.Phys. C57 (1993) 211-218, 1993.
Inspire Record 341575 DOI 10.17182/hepdata.14499
3 data tables

Results from the 'chariot' experiment.

Results from the 'addendum' experiment.

Merged 'chariot' and 'addendum' ratio.. Errors are combined statistics and systematics.


Measurements of R(d) - R(p) and R(Ca) - R(C) in deep inelastic muon scattering

The New Muon collaboration Amaudruz, P. ; Arneodo, M. ; Arvidson, A. ; et al.
Phys.Lett. B294 (1992) 120-126, 1992.
Inspire Record 340582 DOI 10.17182/hepdata.29038
4 data tables

No description provided.

Average overall x values.

No description provided.

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Precision measurement of structure function ratios for Li-6, C-12 and Ca-40

The New Muon collaboration Amaudruz, P. ; Arneodo, M. ; Arvidson, A. ; et al.
Z.Phys. C53 (1992) 73-78, 1992.
Inspire Record 319669 DOI 10.17182/hepdata.14706
3 data tables

Overall normalization error of 0.7%, due to uncertainties in target thickness, not included in the table.

Overall normalization error of 0.8%, due to uncertainties in target thickness, not included in the table.

Overall normalization error of 0.5%, due to uncertainties in target thickness, not included in the table.


Precision measurement of the structure function ratios F2 (He) / F2 (D), F2 (C) / F2 (D) and F2 (Ca) / F2 (D)

The New Muon collaboration Amaudruz, P. ; Arneodo, M. ; Arvidson, A. ; et al.
Z.Phys. C51 (1991) 387-394, 1991.
Inspire Record 314878 DOI 10.17182/hepdata.14935
3 data tables

No description provided.

No description provided.

No description provided.


Measurements of the nucleon structure function in the range $0.002-{\rm GeV}^2 < x < 0.17-{\rm GeV}^2$ and $0.2-GeV^2 < q^2 < 8-GeV^2$ in deuterium, carbon and calcium

The European Muon collaboration Arneodo, M. ; Arvidson, A. ; Aubert, J.J. ; et al.
Nucl.Phys. B333 (1990) 1-47, 1990.
Inspire Record 283347 DOI 10.17182/hepdata.33074
33 data tables

Deuterium data. Overall normalization error of 7 pct not included.

Deuterium data. Overall normalization error of 7 pct not included.

Deuterium data. Overall normalization error of 7 pct not included.

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Shadowing in Deep Inelastic Muon Scattering from Nuclear Targets

The European Muon collaboration Arneodo, M. ; Arvidson, A. ; Aubert, J.J. ; et al.
Phys.Lett. B211 (1988) 493-499, 1988.
Inspire Record 262246 DOI 10.17182/hepdata.29908
4 data tables

VALUES OF Q**2 AT EACH POINT ARE:- 0.52,0.60,0.61,0.61,0.63,0.68,0.90.

VALUES OF Q**2 AT EACH POINT ARE:- 1.09,1.25,1.54,1.74,1.76,1.68,1.71, 2.29.

VALUES OF X AT EACH POINT ARE:- 0.009,0.011,0.010,0.010,0.010,0.011, 0.013,0.015.

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Measurement of the Ratios of Deep Inelastic Muon - Nucleus Cross-Sections on Various Nuclei Compared to Deuterium

The European Muon collaboration Ashman, J. ; Badelek, B. ; Baum, Guenter ; et al.
Phys.Lett. B202 (1988) 603-610, 1988.
Inspire Record 260668 DOI 10.17182/hepdata.29991
3 data tables

Q**2= 5.1,7.8,11.4,14.4,17.3,20.2,24.1,29.8,33.6 GEV**2.

Q**2= 4.4,8.4,13.5,17.9,21.1,24.4,29.5,34.0,40.4 GEV**2.

Q**2= 4.0,7.7,11.1,14.6,17.1,19.8,24.8,32.4 GEV**2.


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.


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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Study of nuclear effects in the determination of nucleon structure functions with heavy targets

The Bologna-CERN-Dubna-Munich-Saclay collaboration Benvenuti, A.C. ; Bollini, D. ; Bruni, G. ; et al.
Conference Paper, 2016.
Inspire Record 207569 DOI 10.17182/hepdata.39514
4 data tables

No description provided.

No description provided.

F2(FE)/F2(DEUT) AVERAGED OVER Q2.

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Measurement of the Interference Structure Function Xg(3) (X) in Muon - Nucleon Scattering

Argento, A. ; Benvenuti, A.C. ; Bollini, D. ; et al.
Phys.Lett. B140 (1984) 142-144, 1984.
Inspire Record 195945 DOI 10.17182/hepdata.13025
3 data tables

No description provided.

No description provided.

No description provided.


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.


The ratio of the nucleon structure functions $F2_n$ for iron and deuterium

The European Muon collaboration Aubert, J.J. ; Bassompierre, G. ; Becks, K.H. ; et al.
Phys.Lett. B123 (1983) 275-278, 1983.
Inspire Record 188925 DOI 10.17182/hepdata.30745
1 data table

RANGE OF Q*2 VARIES WITH X. E.G. AT X=0.05 , 9<Q2<27. AT X=0.65 , 36<Q2<170 GEV**2.