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QUENCHED QCD AT FINITE-DENSITY
被引:43
|
作者
:
KOGUT, JB
论文数:
0
引用数:
0
h-index:
0
机构:
ARGONNE NATL LAB,DIV HIGH ENERGY PHYS,ARGONNE,IL 60439
ARGONNE NATL LAB,DIV HIGH ENERGY PHYS,ARGONNE,IL 60439
KOGUT, JB
[
1
]
LOMBARDO, MP
论文数:
0
引用数:
0
h-index:
0
机构:
ARGONNE NATL LAB,DIV HIGH ENERGY PHYS,ARGONNE,IL 60439
ARGONNE NATL LAB,DIV HIGH ENERGY PHYS,ARGONNE,IL 60439
LOMBARDO, MP
[
1
]
SINCLAIR, DK
论文数:
0
引用数:
0
h-index:
0
机构:
ARGONNE NATL LAB,DIV HIGH ENERGY PHYS,ARGONNE,IL 60439
ARGONNE NATL LAB,DIV HIGH ENERGY PHYS,ARGONNE,IL 60439
SINCLAIR, DK
[
1
]
机构
:
[1]
ARGONNE NATL LAB,DIV HIGH ENERGY PHYS,ARGONNE,IL 60439
来源
:
PHYSICAL REVIEW D
|
1995年
/ 51卷
/ 03期
关键词
:
D O I
:
10.1103/PhysRevD.51.1282
中图分类号
:
P1 [天文学];
学科分类号
:
0704 ;
摘要
:
Simulations of quenched QCD at a relatively small but nonzero chemical potential μ on 32×163 lattices indicate that the nucleon screening mass decreases linearly as μ increases predicting a critical chemical potential of one-third the nucleon mass, mN/3, by extrapolation. The meson spectrum does not change as μ increases over the same range, from zero to mπ/2. Past studies of quenched lattice QCD have suggested that there is phase transition at μ=mπ/2. We discuss a number of technical reasons why standard lattice simulation techniques suffer from greatly enhanced fluctuations and finite size effects for μ ranging from mπ/2 to mN/3. We find evidence for such problems in our simulations, and suggest that they can be surmounted by improved measurement techniques, which should enable us to extend our calculations to the interesting domain mπ/2<μ<mN/3. © 1995 The American Physical Society.
引用
收藏
页码:1282 / 1291
页数:10
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