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that would break baryon number conservation and lepton number conservation individually cancel in such a way that
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Wilczek, Frank; Zee, A. (1979). "Operator analysis of nucleon decay".
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Quantum number; the difference between the baryon and lepton numbers
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419:PMNS matrix
292:Hypercharge
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995:See also
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960:Soudan 2
955:Soudan 1
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608:where a
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272:X-charge
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787:Majoron
753:X boson
534:−
504:Details
496:) of a
214:′
199:Topness
165:Isospin
143:Flavour
101:scholar
76:"B − L"
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950:NUSEX
647:= 0,
632:= 0,
617:= 1,
518:gauge
508:This
387:= 5 (
363:= 2 (
329:= 2 (
181:Charm
108:JSTOR
94:books
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761:U(1)
678:via
656:The
651:= –1
625:pion
586:The
529:U(1)
521:U(1)
80:news
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930:HPW
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653:).
636:= 0
621:= 0
551:If
544:or
462:In
380:+ 2
303:= (
253:or
171:or
63:by
18:B-L
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