K. Vansyoc

发表

Prototype studies and design considerations for the CLAS Region 2 drift chambers

B. Raue, L. Weinstein, G. Dodge, 1998 .

Charged pion form factor between Q2=0.60 and 2.45 GeV2. II. Determination of, and results for, the pion form factor

K. Assamagan, O. Baker, G. Smith, 2008, 0809.3052.

The CLAS drift chamber system

R. W. Major, J. Mueller, M. Kossov, 2000 .

Measurement of the charged pion electromagnetic form factor.

K., K. Assamagan, O. Baker, 2000, Physical review letters.

Charged pion form factor between $Q^2$=0.60 and 2.45 GeV$^2$. I. Measurements of the cross section for the ${^1}$H($e,e'\pi^+$)$n$ reaction

K. Assamagan, O. Baker, G. Smith, 2008, 0809.3161.

Tensor polarization in elastic electron-deuteron scattering to the highest possible momentum transfers

L. Eyraud, P. Markowitz, S. Mtingwa, 1998 .

Phenomenology of the deuteron electromagnetic form factors

L. Eyraud, P. Markowitz, S. Mtingwa, 2000, nucl-ex/0002003.

Determination of the pion charge form factor for Q 2 = 0.60 1.60 GeV 2

K. Assamagan, O. Baker, R. V. Meer, 2006, nucl-ex/0607007.

Charged pion form factor between Q2=0.60 and 2.45 GeV2. II. Determination of, and results for, the pion form factor

K. Assamagan, O. Baker, G. Smith, 2008 .