-
15
-
-
33750567914
-
-
E. Abdalla, M. C. B. Abdalla, and K. D. Rothe, 2 Dimensional Quantum Field Theory (World Scientific, Singapore, 1991).
-
Singapore
, vol.1991
-
-
Abdalla, E.1
Abdalla, M.C.B.2
Rothe, K.D.3
Scientific, D.Q.4
-
16
-
-
33750562675
-
-
note
-
When we apply this formula in Eq. (2), we must pay care to zero modes of D. Generally this point is related to the fixing of local (gauge) symmetry and the regularization of the infrared behavior. In the present case, there exists no problem in this respect. See Chap. IV of Ref. [15].
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-
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-
20
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-
26744450269
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-
Phys. Rev. Lett. 44, 1733 (1980);
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(1980)
Phys. Rev. Lett.
, vol.44
, pp. 1733
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-
-
21
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-
4243648786
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-
Phys. Rev. D 21, 2848 (1980);
-
(1980)
Phys. Rev. D
, vol.21
, pp. 2848
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-
-
22
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-
33744577255
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-
Phys. Rev. D 22, 1499(E) (1980).
-
(1980)
Phys. Rev. D
, vol.22
, pp. 1499
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-
-
25
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-
85107712855
-
-
note
-
a) in (1 +4)-dimensional Minkowski space.
-
-
-
-
26
-
-
33750555876
-
-
note
-
Here we introduce two independent regularization parameters M and A/' in order to stress that the two domains are defined not by (the sign of) the (1+4)-dimensional fermion mass but by the relation (14). This point distinguishes the present formalism from the original overlap formalism. We will soon take M = M' for simplicity.
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-
-
-
29
-
-
85107714874
-
-
a).
-
a).
-
-
-
-
30
-
-
85107712057
-
-
note
-
μ.
-
-
-
-
31
-
-
85107714473
-
-
note
-
5 + ik.
-
-
-
-
32
-
-
85107713881
-
-
note
-
1 (circle). In the present case, however, the extra space can not be compactified since it is known, in the lattice formalism, that the fermion doubler appears in the case when the periodic boundary condition is imposed on the extra space [4].
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-
-
-
33
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-
85107713320
-
-
note
-
μ|→ + ∞ that of the ultraviolet regularization. In the sense that both the ultraviolet and the infrared cutoffs exist, the present regularization is similar to the lattice regularization.
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-
-
-
34
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-
0002110725
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-
hep-lat/9903024
-
A symmetry with domain wall fermions" hep-lat/9903024.
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A Symmetry with Domain Wall Fermions
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-
Vranas, P.1
Chen, P.2
Christ, N.3
Fleming, G.4
Kaehler, A.5
Malureanu, C.6
Mawhinney, R.7
Siegert, G.8
Sui, C.9
Wu, L.10
Zhestkov, Y.11
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35
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-
85107711999
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-
0 integral in Eq. (37), and the final anomaly result depends on it
-
0 integral in Eq. (37), and the final anomaly result depends on it.
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-
-
-
36
-
-
85107714837
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-
note
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2/M≤1. In this sense, the third stage condition (29) is used in a loosened way. We regard it as a part of regularization. The same thing can be said for the evaluation of Eq. (44).
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