84,667 research outputs found

    The Schrodinger-like Equation for a Nonrelativistic Electron in a Photon Field of Arbitrary Intensity

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    The ordinary Schrodinger equation with minimal coupling for a nonrelativistic electron interacting with a single-mode photon field is not satisfied by the nonrelativistic limit of the exact solutions to the corresponding Dirac equation. A Schrodinger-like equation valid for arbitrary photon intensity is derived from the Dirac equation without the weak-field assumption. The "eigenvalue" in the new equation is an operator in a Cartan subalgebra. An approximation consistent with the nonrelativistic energy level derived from its relativistic value replaces the "eigenvalue" operator by an ordinary number, recovering the ordinary Schrodinger eigenvalue equation used in the formal scattering formalism. The Schrodinger-like equation for the multimode case is also presented.Comment: Tex file, 13 pages, no figur

    On the least common multiple of qq-binomial coefficients

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    In this paper, we prove the following identity \lcm({n\brack 0}_q,{n\brack 1}_q,...,{n\brack n}_q) =\frac{\lcm([1]_q,[2]_q,...,[n+1]_q)}{[n+1]_q}, where [nk]q{n\brack k}_q denotes the qq-binomial coefficient and [n]q=1qn1q[n]_q=\frac{1-q^n}{1-q}. This result is a qq-analogue of an identity of Farhi [Amer. Math. Monthly, November (2009)].Comment: 5 page

    Factors of sums and alternating sums involving binomial coefficients and powers of integers

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    We study divisibility properties of certain sums and alternating sums involving binomial coefficients and powers of integers. For example, we prove that for all positive integers n1,...,nmn_1,..., n_m, nm+1=n1n_{m+1}=n_1, and any nonnegative integer rr, there holds {align*} \sum_{k=0}^{n_1}\epsilon^k (2k+1)^{2r+1}\prod_{i=1}^{m} {n_i+n_{i+1}+1\choose n_i-k} \equiv 0 \mod (n_1+n_m+1){n_1+n_m\choose n_1}, {align*} and conjecture that for any nonnegative integer rr and positive integer ss such that r+sr+s is odd, k=0nϵk(2k+1)r((2nnk)(2nnk1))s0mod(2nn), \sum_{k=0}^{n}\epsilon ^k (2k+1)^{r}({2n\choose n-k}-{2n\choose n-k-1})^{s} \equiv 0 \mod{{2n\choose n}}, where ϵ=±1\epsilon=\pm 1.Comment: 14 pages, to appear in Int. J. Number Theor

    Metastable helium molecules as tracers in superfluid liquid 4^{4}He

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    Metastable helium molecules generated in a discharge near a sharp tungsten tip operated in either pulsed mode or continuous field-emission mode in superfluid liquid 4^{4}He are imaged using a laser-induced-fluorescence technique. By pulsing the tip, a small cloud of He2_{2}^{*} molecules is produced. At 2.0 K, the molecules in the liquid follow the motion of the normal fluid. We can determine the normal-fluid velocity in a heat-induced counterflow by tracing the position of a single molecule cloud. As we run the tip in continuous field-emission mode, a normal-fluid jet from the tip is generated and molecules are entrained in the jet. A focused 910 nm pump laser pulse is used to drive a small group of molecules to the vibrational a(1)a(1) state. Subsequent imaging of the tagged a(1)a(1) molecules with an expanded 925 nm probe laser pulse allows us to measure the velocity of the normal fluid. The techniques we developed demonstrate for the first time the ability to trace the normal-fluid component in superfluid helium using angstrom-sized particles.Comment: 4 pages, 7 figures. Submitted to Phys. Rev. Let
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