General Fierz-type identities are examined and their well-known connection with completeness relations in matrix vector spaces is shown. In particular, I derive the chiral Fierz identities in a simple and systematic way by using a chiral basis for the complex 4×4 matrices. Other completeness relations for the fundamental representations of SU(N) algebras can be extracted using the same reasoning.

1.
M.
Fierz
, “
Zur Fermischen Theorie des β-Zerfalls
,”
Z. Phys.
104
,
553
565
(
1937
).
2.
J. F.
Donoghue
,
E.
Golowich
, and
B. R.
Holstein
,
Dynamics of the Standard Model
(
Cambridge University Press
,
1994
), pp.
217
and
221
.
3.
J. D.
Bjorken
and
S. D.
Drell
,
Relativistic Quantum Mechanics
(
McGraw-Hill
, New York,
1965
).
4.
Y.
Takahashi
, “
The Fierz identities
,” in
Progress in Quantum Field Theory
, edited by
H.
Ezawa
and
S.
Kamefuchi
(
North-Holland
, Amsterdam,
1986
), p.
121
.
5.
J. F.
Nieves
and
P. B.
Pal
, “
Generalized Fierz identities
,”
Am. J. Phys.
72
,
1100
1108
(
2004
).
6.
R.
Mohapatra
and
P.
Pal
,
Massive Neutrinos in Physics and Astrophysics
(
World Scientific
, Singapore,
1991
), pp.
165
70
.
7.
The surprising implications and experimental evidences for neutrino oscillations can be found in
W. C.
Haxton
and
B. R.
Holstein
, “
Neutrino physics
,”
Am. J. Phys.
68
,
15
32
(
2000
);
also
W. C.
Haxton
and
B. R.
Holstein
, “
Neutrino physics: An update
,”
Am. J. Phys.
72
,
18
24
(
2004
);
see also
M. C.
Gonzalez-Garcia
and
Y.
Nir
, “
Neutrino masses and mixing: Evidence and implications
,”
Rev. Mod. Phys.
75
,
345
402
(
2003
).
8.
See any linear algebra book, for example,
I. M.
Gel’fand
,
Lectures on Linear Algebra
(
Interscience
, New York,
1961
).
9.

Any operation applied to an element in the vector space must result in another element of the vector space.

10.

MN(C) may be considered as a 2N2 dimensional vector space if spanned by N2 real matrices and N2 purely complex matrices with real expansion coefficients only, that is, over the reals R.

11.
See
C.
Itzykson
and
J. B.
Zuber
,
Quantum Field Theory
(
McGraw-Hill
, New York,
1980
), p.
516
, for an explicit representation of Gell-Mann matrices.
12.

The SU(2) and SU(3) generators are {12σi} and {12λa}, respectively.

13.

I will denote as Dirac bilinears the proper bilinears containing the two spinors as well as the associated matrices alone, because the Fierz identities do not depend on the spinors involved.

14.

The lowering of space-time indices is equivalent to the hermitian conjugation operation.

15.
See Ref. 11, Appendix.
16.

These identities were used to get from Eq. (1) to Eq. (2) with a sign difference due to the anticommutation of fermion fields.

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