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Chanchal K. Majumdar

Researcher at S.N. Bose National Centre for Basic Sciences

Publications -  56
Citations -  1053

Chanchal K. Majumdar is an academic researcher from S.N. Bose National Centre for Basic Sciences. The author has contributed to research in topics: Bound state & Hamiltonian (quantum mechanics). The author has an hindex of 10, co-authored 56 publications receiving 974 citations. Previous affiliations of Chanchal K. Majumdar include University of California, San Diego & University of Calcutta.

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On Next‐Nearest‐Neighbor Interaction in Linear Chain. II

TL;DR: In this paper, the ground state properties of the Hamiltonian H = 12J ∑ i=1N σi·σi+1 + 12Jα ∑ n σI·σI+2 for both signs of J and −1 ≤ α ≤ 1 to gain insight into the stability of the ground states with nearest-neighbor interactions only (α = 0) in the presence of the next-nearest-nighbor interaction.
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Continuity between bound and unbound states in a fermi gas

TL;DR: In this article, a soluble model of a gas of independent fermions in the presence of an attractive localized potential was considered, and it was shown that the properties of the system as a whole are smooth (analytic) functions of the potential.
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Crystallite size dependence on the magnetic properties of nanocrystalline magnetite powders

TL;DR: In this article, single phase magnetite powders with crystallite sizes ranging from 8-50 nm were synthesized and studied using X-ray diffraction and Mossbauer spectroscopy.
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An X-ray diffraction and Mossbauer study of nano-crystalline Fe2O3–Cr2O3 solid solutions

TL;DR: A series of gels with nominal composition Fe2−xCrxO3 (x=0-2) was prepared at room temperature by an inorganic sol-gel route and studied by X-ray diffraction and Mossbauer spectroscopy.
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Two Contributions to the Theory of Annihilation of Positrons in Metals. I. Determination of the True Fermi Surface

TL;DR: The theory of positron annihilation in metals, including electron-positron and electron-electron interaction, is discussed in this article, where it is established that a sharp "break" in the angular-correlation curve of the two $\ensuremath{\gamma}$ rays resulting from the singlet-state annihilation occurs at precisely those angles where it should be expected in the absence of electron positron interaction.