23,822 research outputs found

    The 13-C(p,d) Reaction at 120 MeV

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    This research was sponsored by the National Science Foundation Grant NSF PHY 87-1440

    Spectroscopy of η\eta'-nucleus bound states at GSI and FAIR --- very preliminary results and future prospects ---

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    The possible existence of \eta'-nucleus bound states has been put forward through theoretical and experimental studies. It is strongly related to the \eta' mass at finite density, which is expected to be reduced because of the interplay between the UA(1)U_A(1) anomaly and partial restoration of chiral symmetry. The investigation of the C(p,d) reaction at GSI and FAIR, as well as an overview of the experimental program at GSI and future plans at FAIR are discussed.Comment: 7 pages, 3 figures; talk at the International Conference on Exotic Atoms and Related Topics (EXA2014), Vienna, Austria, 15-19 September 2014. in Hyperfine Interactions (2015

    Parity-Affected Superconductivity in Ultrasmall Metallic Grains

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    We investigate the breakdown of BCS superconductivity in {\em ultra}\/small metallic grains as a function of particle size (characterized by the mean spacing dd between discrete electronic eigenstates), and the parity (PP = even/odd) of the number of electrons on the island. Assuming equally spaced levels, we solve the parity-dependent BCS gap equation for the order parameter ΔP(d,T)\Delta_P (d,T). Both the T=0T=0 critical level spacing dc,Pd_{c,P} and the critical temperature Tc,P(d)T_{c,P} (d) at which ΔP=0\Delta_P = 0 are parity dependent, and both are so much smaller in the odd than the even case that these differences should be measurable in current experiments.Comment: 4 pages RevTeX, 1 encapsulated postscript figure, submitted to Physical Review Letter

    Berezin-type quantization on even-dimensional compact manifolds

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    In this article we show that a Berezin-type quantization can be achieved on a compact even dimensional manifold M2dM^{2d} by removing a skeleton M0M_0 of lower dimension such that what remains is diffeomorphic to R2d{\mathbb R}^{2d} which we identify with Cd{\mathbb C}^d and embed in CPd{\mathbb C}P^d. A local Poisson structure and Berezin-type quantization are induced from CPd{\mathbb C}P^d. We have a Hilbert space with a reproducing kernel. The symbols of bounded linear operators on the Hilbert space have a star product which satisfies the correspondence principle outside a set of measure zero. This construction depends on the diffeomorphism. However, suppose X=MM0X= M \setminus M_0 has a complex structure and we have from XX0X \setminus X_0, (X0X_0 a set of measure zero or empty) a biholomorphism from it to CdN0{\mathbb C}^d \setminus N_0, (where N0N_0 is of measure zero or empty). As before we embed CdN0{\mathbb C}^d \setminus N_0 in Cd{\mathbb C}^d and then into CPd{\mathbb C}P^d and we have a Berezin-type quantization induced from CPd{\mathbb C}P^d. If we use another biholomorphism, we have a map of the two Hilbert spaces under consideration such that the reproducing kernel of one maps to the reproducing kernel of the other and we have an equivalent quantization. We have a similar construction where we consider an arbitrary complex manifold and use local coordinates to induce the quantization from CPd{\mathbb C}P^d. We study the possibility of defining a global Berezin quantization on compact complex manifolds. We give a defintion of pullback Toeplitz operators and exhibit Toeplitz quantization of compact even dimensional manifolds after removing a set of measure zero. Next we give a simple construction of pullback coherent states on compact smooth manifolds which are simplified versions of those defined in an earlier work by the authors

    List decoding Reed-Muller codes over small fields

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    The list decoding problem for a code asks for the maximal radius up to which any ball of that radius contains only a constant number of codewords. The list decoding radius is not well understood even for well studied codes, like Reed-Solomon or Reed-Muller codes. Fix a finite field F\mathbb{F}. The Reed-Muller code RMF(n,d)\mathrm{RM}_{\mathbb{F}}(n,d) is defined by nn-variate degree-dd polynomials over F\mathbb{F}. In this work, we study the list decoding radius of Reed-Muller codes over a constant prime field F=Fp\mathbb{F}=\mathbb{F}_p, constant degree dd and large nn. We show that the list decoding radius is equal to the minimal distance of the code. That is, if we denote by δ(d)\delta(d) the normalized minimal distance of RMF(n,d)\mathrm{RM}_{\mathbb{F}}(n,d), then the number of codewords in any ball of radius δ(d)ε\delta(d)-\varepsilon is bounded by c=c(p,d,ε)c=c(p,d,\varepsilon) independent of nn. This resolves a conjecture of Gopalan-Klivans-Zuckerman [STOC 2008], who among other results proved it in the special case of F=F2\mathbb{F}=\mathbb{F}_2; and extends the work of Gopalan [FOCS 2010] who proved the conjecture in the case of d=2d=2. We also analyse the number of codewords in balls of radius exceeding the minimal distance of the code. For ede \leq d, we show that the number of codewords of RMF(n,d)\mathrm{RM}_{\mathbb{F}}(n,d) in a ball of radius δ(e)ε\delta(e) - \varepsilon is bounded by exp(cnde)\exp(c \cdot n^{d-e}), where c=c(p,d,ε)c=c(p,d,\varepsilon) is independent of nn. The dependence on nn is tight. This extends the work of Kaufman-Lovett-Porat [IEEE Inf. Theory 2012] who proved similar bounds over F2\mathbb{F}_2. The proof relies on several new ingredients: an extension of the Frieze-Kannan weak regularity to general function spaces, higher-order Fourier analysis, and an extension of the Schwartz-Zippel lemma to compositions of polynomials.Comment: fixed a bug in the proof of claim 5.6 (now lemma 5.5

    Theoretical studies in the molecular Platonic solids: Pure and mixed carbon, nitrogen, phosphorus, and silicon tetrahedranes

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    Calculations were conducted at the G4MP2 and G4 composite method levels of theory on the 35 potential carbon, nitrogen, silicon, and phosphorus tetrahedrane derivatives with the general form C~a~N~b~Si~c~P~d~H~(4-b-d)~ (where a+b+c+d=4). At both levels of theory, optimized electronic ground state neutral singlet gas phase (298.15 K, 1 atm) geometries were obtained for 24 of the 35 possible C/N/Si/P tetrahedrane derivatives. Corresponding enthalpies of formation were calculated using the atomization method. Triplet state neutral tetrahedron starting geometries for all compounds either resulted in cage opening or failed to converge. Only 9 cationic and 3 anionic forms converged to stable geometries that retained the tetrahedron cage and were absent imaginary frequencies, thereby allowing the calculation of adiabatic ionization energies and electron affinities
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