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1.
Effects of Quenching in $\Delta$I=1/2 Kaon Decays / Lin, C J D ; Martinelli, G ; Pallante, E ; Sachrajda, Christopher T C ; Villadoro, Giovanni
We present the inconsistencies which arise in quenched QCD in $\Delta I=1/2$ non-leptonic kaon decays using chiral perturbation theory (ChPT) to one loop. In particular we discuss how the lack of unitarity of the quenched theory invalidates the usual methods for the extraction of matrix elements from correlation functions..
hep-lat/0209107; CERN-TH-2002-235; SHEP-2002-19.- Geneva : CERN, 2003 - 3 p. - Published in : Nucl. Phys. B, Proc. Suppl. 119 (2003) 371-373 Access to fulltext document: PDF; External link: hep-lat/0209107 PDF
In : 20th International Symposium on Lattice Field Theory, Cambridge, MA, USA, 24 - 29 Jun 2002, pp.371-373
2.
$K^{+}\to\pi^{+}\pi^{0}$ decays at next-to-leading order in the chiral expansion on finite volumes / Lin, C J D ; Martinelli, G ; Pallante, E ; Sachrajda, Christopher T C ; Villadoro, Giovanni
We present the ingredients for determining $K^{+}\to\pi^{+}\pi^{0}$ matrix elements via the combination of lattice QCD and chiral perturbation theory ($\chi$PT). By simulating these matrix elements at unphysical kinematics, it is possible to determine all the low-energy constants (LECs) for constructing the physical $K^{+}\to\pi^{+}\pi^{0}$ amplitudes at next-to-leading order (NLO) in the chiral expansion. [...]
hep-lat/0209020; SHEP-2002-18; CERN-TH-2002-234.- Southampton : Southampton Univ. Phys. Dept., 2003 - 3 p. - Published in : Nucl. Phys. B, Proc. Suppl. 119 (2003) 383-385 Access to fulltext document: PDF; External link: hep-lat/0209020 PDF
In : 20th International Symposium on Lattice Field Theory, Cambridge, MA, USA, 24 - 29 Jun 2002, pp.383-385
3.
$K^{+} \to pi^{+} pi^{0}$ Decays on Finite Volumes and at Next-to-Leading Order in the Chiral Expansion / Lin, C J D ; Martinelli, G ; Pallante, E ; Sachrajda, Christopher T C ; Villadoro, Giovanni
We present the ingredients necessary for the determination of physical K->pi pi decay amplitudes for Delta I=3/2 transitions, from lattice simulations at unphysical kinematics and the use of chiral perturbation theory at next-to-leading order. In particular we derive the expressions for the matrix elements <pi pi(I=2)|O_W|K>, where O_W is one of the operators appearing in the Delta S=1 weak Hamiltonian, in terms of low-energy constants at next-to-leading order in the chiral expansion. [...]
hep-lat/0208007; CERN-TH-2002-130; ROMA-1-1337; SHEP-2002-13; SISSA-2002-47-EP.- Geneva : CERN, 2003 - 57 p. - Published in : Nucl. Phys. B 650 (2003) 301-355 Access to fulltext document: PDF; External link: hep-lat/0208007 PDF

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197 Lin, C
3 Lin, C H
1 Lin, C -C
1 Lin, C -H
5 Lin, C -J
2 Lin, C -J D
28 Lin, C -J David
1 Lin, C -L
1 Lin, C A
14 Lin, C C
2 Lin, C C Y
41 Lin, C D
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100 Lin, C H
1 Lin, C I
37 Lin, C J
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1 Lin, C K
2 Lin, C L
1 Lin, C M
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172 Lin, C S
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61 Lin, C Y
1 Lin, C Z
6 Lin, C  H
2 Lin, C-J
3 Lin, C-J.S.
9 Lin, C-Y.
53 Lin, C.
1 Lin, C. -J. David
1 Lin, C.-C.
2 Lin, C.-J.
4 Lin, C.-J. David
2 Lin, C.-J.David
1 Lin, C.-h.
133 Lin, C.H.
103 Lin, C.J.
3 Lin, C.J.David
17 Lin, C.S.
1 Lin, C.X.
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2 Lin, CD
1 Lin, CJDavid
1 Lin, Calvin
1 Lin, Carol Sze Ki
3 Lin, Carol Yeh-Yun
1 Lin, Chaney
14 Lin, Chang-Shou
1 Lin, Chang-Yi
14 Lin, Chang-shou
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2 Lin, Charles
5 Lin, Che
4 Lin, Che-Yun
4 Lin, Che-yun
1 Lin, Chen
1 Lin, Chen-Hui Jerry
1 Lin, Chen-Ying
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4 Lin, Cheng
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1 Lin, Ching-Fuh
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5 Lin, Ching-Lung
1 Lin, Ching-Ting
1 Lin, Ching-Yung
2 Lin, Chinlon
3 Lin, Chiun-Yan
1 Lin, Chris
5 Lin, Chris L
2 Lin, Christopher
1 Lin, Christy
1 Lin, Chuan-Yu
3 Lin, Chuandong
2 Lin, Chuang
144 Lin, Chuangxin
489 Lin, Chuanzhe
7 Lin, Chun C
2 Lin, Chun C 0
3 Lin, Chun-Cheng
1 Lin, Chun-Chi
1 Lin, Chun-Wei
6 Lin, Chun-Yen
8 Lin, Chun-Yu
1 Lin, Chun-Yueh
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27 Lin, Chunshan
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3 Lin, Chunyu
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1 lin, Cen
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