2007
DOI: 10.1007/s10773-007-9573-1
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Playing with Numbers, with Fermions and Bosons

Abstract: We construct nonlinear maps which realize the fermionization of bosons and the bosonization of fermions with the view of obtaining states coding naturally integers in standard or in binary basis. Specifically, with reference to spin 1 2 systems, we derive raising and lowering bosonic operators in terms of standard fermionic operators and vice versa. The crucial role of multiboson operators in the whole construction is emphasized.

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Cited by 1 publication
(4 citation statements)
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“…[5] for spin Omitting computational details, one finds that S (ℓ) = 1 √γ ℓ + 1 a ℓ satisfies both conditions (14); a ℓ andγ ℓ denote the annihilation and the number operators of the (ℓ+1)-th slot, a ℓ |γ ℓ = √ γ ℓ |γ ℓ −1 ,γ ℓ |γ ℓ = γ ℓ |γ ℓ . However, the raising slot operator S † (ℓ) verifies only the first of conditions (15) while the second one needs somehow to be forced .…”
Section: The Slot Operatorsmentioning
confidence: 99%
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“…[5] for spin Omitting computational details, one finds that S (ℓ) = 1 √γ ℓ + 1 a ℓ satisfies both conditions (14); a ℓ andγ ℓ denote the annihilation and the number operators of the (ℓ+1)-th slot, a ℓ |γ ℓ = √ γ ℓ |γ ℓ −1 ,γ ℓ |γ ℓ = γ ℓ |γ ℓ . However, the raising slot operator S † (ℓ) verifies only the first of conditions (15) while the second one needs somehow to be forced .…”
Section: The Slot Operatorsmentioning
confidence: 99%
“…One derives the expression of S (ℓ) extending the formulation reported in Ref. [5] for spin 1 2 systems to general spin j systems. Specifically, S (ℓ) and S † (ℓ) are expressed in terms of the spin j representations of the generators J − and J + = J † − of the su(2) algebra {J + , J − , J z }, [J + , J − ] = 2J z , [J z , J ± ] = ±J ± , the standard basis |j, m , −j ≤ m ≤ j, being replaced with the number basis through the Holstein-Primakoff representation of su(2) [10].…”
Section: The Slot Operatorsmentioning
confidence: 99%
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