Previous Publications

Review papers:

• Run I Tevatron W Mass measurement: Annual Review: Ann. Rev. Nucl. Part. Sci. 58 (2008) 147.
• Run II Tevatron W Mass measurement: Annual Review: Ann. Rev. Nucl. Part. Sci. 50 (2000) 207.
• Tevatron Inclusive Jet and Di-Jet Production: Annual Review: Ann. Rev. Nucl. Part. Sci. 49 (1999) 633.
• Electroweak Studies at Z Factories: Annual Review: Ann. Rev. Nucl. Part. Sci. 48 (1998) 463.
• QCD Tests at the Tevatron and SPS: Annual Review: Ann. Rev. Nucl. Part. Sci. 43 (1993) 585.
• Hadron Collider Physics: Annual Review: Ann. Rev. Nucl. Part. Sci. 41 (1991) 97.

Discovery of the W bosons (UA1/UA2):

• UA1: Phys. Lett. B122 (1983) 103.
• UA2: Phys. Lett. B122 (1983) 476.

Discovery of the Z boson (UA1/UA2):

• UA1: Phys. Lett. B126 (1983) 398.
• UA2: Phys. Lett. B129 (1983) 130.

Precise measurement of the W mass by UA1:

• UA1: Z. Phys. C44 (1989) 15.

Precise measurement of the W mass by UA2 (First with an accuracy of 1GeV):

• UA2: Phys. Lett. B241 (1990) 150.

Tevatron Run I (1991-1995) results on the W mass with a precision of 100MeV:

• CDF: Phys. Rev. D64 (2001) 052001.
• D0: Phys. Rev. D58 (1998) 092003.
• D0: Phys. Rev. D58 (1998) 012002.
• D0: Phys. Rev. D62 (2000) 092006.
• D0: Phys. Rev. D66 (2002) 012001.

Pawel Nadolsky, RhicBos, predictions for STAR

• Longitudinal parity-violating asymmetry in W-boson mediated jet pair production (Presentation),
  E. Berger and P. Nadolsky, Phys. Rev. D78, 114010 (2008)

Papers about ubar/dbar x-section

• M. Grosse-Perdekamp for PHENIX

1. Computation of AL from RHICBOS - Bernd
   
   
   Unknown macro: {latex}

   ~
   
   L0 interpretation of parity violating $A_L$ for Ws

   1) definition of sign of $A_L$:
   \begin

   Unknown macro: {equation}

   A_L=\frac

   Unknown macro: {dsigma^+ - dsigma^-}

   Unknown macro: {dsigma^+ + dsigma^-}

   \end

   
   Explore limits at $y=0, x_a=x_b=x$
   \begin

   Unknown macro: {equation}

   A^

   Unknown macro: {W+}

   _L=\frac{u\Delta\bar

   Unknown macro: {d}

   - \bar

   \Delta u}{2u\bar

   Unknown macro: {d}

   }; \;\;\;
   A^

   Unknown macro: {W-}

   _L=\frac{d\Delta\bar

   Unknown macro: {u}

   - \bar

   \Delta d}{2d\bar

   Unknown macro: {u}

   }
   \end

   from this follows:
   \begin

   Unknown macro: {equation}

   A^

   Unknown macro: {W+}

   _L=\frac

   Unknown macro: {1}

   Unknown macro: {2}

   (\frac{\Delta\bar{d}}{\bar{d}} - \frac

   Unknown macro: {Delta u }

   Unknown macro: {u}

   ); \;\;\; A^

   _L<0 \;\; for \;\;\Delta u>0
   \end

   and:
   \begin

   Unknown macro: {equation}

   A^

   Unknown macro: {W-}

   _L=\frac

   Unknown macro: {1}

   Unknown macro: {2}

   (\frac{\Delta\bar{u}}{\bar{u}} - \frac

   Unknown macro: {Delta d }

   Unknown macro: {d}

   ); \;\;\; A^

   _L>0 \;\; for \;\;\Delta d<0
   \end