Page History

h5. Review papers: aa

* Run I Tevatron W Mass measurement: [Annual Review: Ann. Rev. Nucl. Part. Sci. 58 (2008) 147. | ^Ann.Rev.Nucl.Part.Sci.58.147.2008.pdf] 
* Run II Tevatron W Mass measurement: [Annual Review: Ann. Rev. Nucl. Part. Sci. 50 (2000) 207. | ^Ann.Rev.Nucl.Part.Sci.50.207.2000.pdf]
* Tevatron Inclusive Jet and Di-Jet Production: [Annual Review: Ann. Rev. Nucl. Part. Sci. 49 (1999) 633. | ^Ann.Rev.Nucl.Part.Sci.49.633.1999.pdf]
* Electroweak Studies at Z Factories: [Annual Review: Ann. Rev. Nucl. Part. Sci. 48 (1998) 463. | ^Ann.Rev.Nucl.Part.Sci.48.463.1998.pdf]
* QCD Tests at the Tevatron and SPS: [Annual Review: Ann. Rev. Nucl. Part. Sci. 43 (1993) 585. | ^Ann.Rev.Nucl.Part.Sci.43.585.1993.pdf]
* Hadron Collider Physics: [Annual Review: Ann. Rev. Nucl. Part. Sci. 41 (1991) 97. | ^Ann.Rev.Nucl.Part.Sci.41.97.1991.pdf]

h5. Discovery of the W bosons (UA1/UA2):

* UA1: [Phys. Lett. B122 (1983) 103. | ^Phys.Lett.B122.103.1983.pdf]
* UA2: [Phys. Lett. B122 (1983) 476. | ^Phys.Lett.B122.476.1983.pdf]

h5. Discovery of the Z boson (UA1/UA2):

* UA1: [Phys. Lett. B126 (1983) 398. | ^Phys.Lett.B126.398.1983.pdf]
* UA2: [Phys. Lett. B129 (1983) 130. | ^Phys.Lett.B129.130.1983.pdf]

h5. Precise measurement of the W mass by UA1: 

* UA1: [Z. Phys. C44 (1989) 15. | ^Z.Phys.C44.15.1989.pdf]

h5. Precise measurement of the W mass by UA2 (First with an accuracy of 1GeV): 

* UA2: [Phys. Lett. B241 (1990) 150. | ^Phys.Lett.B241.150.1990.pdf]

h5. Tevatron Run I (1991-1995) results on the W mass with a precision of 100MeV:

* CDF: [Phys. Rev. D64 (2001) 052001. | ^Phys.Rev.D64.052001.2001.pdf]
* D0: [Phys. Rev. D58 (1998) 092003. | ^Phys.Rev.D58.092003.2003.pdf]
* D0: [Phys. Rev. D58 (1998) 012002. | ^Phys.Rev.D58.012002.1998.pdf]
* D0: [Phys. Rev. D62 (2000) 092006. | ^Phys.Rev.D62.092006.2000.pdf]
* D0: [Phys. Rev. D66 (2002) 012001. | ^Phys.Rev.D66.012001.2002.pdf]

h5. Pawel Nadolsky, RhicBos, predictions for STAR

* *Longitudinal parity-violating asymmetry in W-boson mediated jet pair production* ([Presentation|^pavel1.pdf]),
\\  [E. Berger and P. Nadolsky, Phys. Rev. D78, 114010 (2008)|^Phys.rev.D78.114010.2008.pdf]


h5. Papers about ubar/dbar x-section

* [M. Grosse-Perdekamp for PHENIX|http://arxiv.org/pdf/0905.3783v2]

h5. Computation of AL from RHICBOS - Bernd

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L0 interpretation of parity violating $A_L$ for Ws

1) definition of sign of $A_L$:
\begin{equation}
A_L=\frac{d\sigma^+ - d\sigma^-}{d\sigma^+ + d\sigma^-}
\end{equation}
\\
Explore limits at $y=0, x_a=x_b=x$
\begin{equation}
A^{W+}_L=\frac{u(x)\Delta\bar{d}(x) - \bar{d}(x)\Delta u(x)}{2u(x)\bar{d}(x)}; \;\;\;
A^{W-}_L=\frac{d(x)\Delta\bar{u}(x) - \bar{u}(x)\Delta d(x)}{2d(x)\bar{u}(x)}\\
\end{equation}
from this follows:
\begin{equation}
A^{W+}_L=\frac{1}{2}(\frac{\Delta\bar{d}}{\bar{d}}(x) - \frac{\Delta u }{u}(x)); \;\;\; A^{W+}_L<0 \;\; for \;\;\Delta u>0
\end{equation}
and:
\begin{equation}
A^{W-}_L=\frac{1}{2}(\frac{\Delta\bar{u}}{\bar{u}}(x) - \frac{\Delta d }{d}(x)); \;\;\; A^{W-}_L>0 \;\; for \;\;\Delta d<0
\end{equation}

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