Deposits of clastic carbonate-dominated (calciclastic) sedimentary slope systems in the rock record have been identified mostly as linearly-consistent carbonate apron deposits, even though most ancient clastic carbonate slope deposits fit the submarine fan systems better. Calciclastic submarine fans are consequently rarely described and are poorly understood. Subsequently, very little is known especially in mud-dominated calciclastic submarine fan systems. Presented in this study are a sedimentological core and petrographic characterisation of samples from eleven boreholes from the Lower Carboniferous of Bowland Basin (Northwest England) that reveals a >250 m thick calciturbidite complex deposited in a calciclastic submarine fan setting. Seven facies are recognised from core and thin section characterisation and are grouped into three carbonate turbidite sequences. They include: 1) Calciturbidites, comprising mostly of highto low-density, wavy-laminated bioclast-rich facies; 2) low-density densite mudstones which are characterised by planar laminated and unlaminated muddominated facies; and 3) Calcidebrites which are muddy or hyper-concentrated debrisflow deposits occurring as poorly-sorted, chaotic, mud-supported floatstones. These

Phd by thesis

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Table Of Integrals Series And Products

Adopted values for the reduced electric quadrupole transition probability, B(E2)↑, from the ground state to the first-excited 2+ state of even–even nuclides are given in Table I. Values of τ, the mean life of the 2+ state; E, the energy; and β, the quadrupole deformation parameter, are also listed there. The ratio of β to the value expected from the single-particle model is presented. The intrinsic quadrupole moment, Q0, is deduced from the B(E2)↑ value. The product E×B(E2)↑ is expressed as a percentage of the energy-weighted total and isoscalar E2 sum-rule strengths.

Table II presents the data on which Table I is based, namely the experimental results for B(E2)↑ values with quoted uncertainties. Information is also given on the quantity measured and the method used. The literature has been covered to November 2000.

The adopted B(E2)↑ values are compared in Table III with the values given by systematics and by various theoretical models. Predictions of unmeasured B(E2)↑ values are also given in Table III.

Transition probability from the ground to the first-excited 2^+ state of even-even nuclides

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Theory Of Simple Liquids

The interacting boson model.

In this paper, Davydov–Chaban approach to study collective motion of atomic nuclei has been mentioned in detail. First by considering a shifted Killingbeck potential, we obtain the wave function of such system by taking an ansatz method. Then we consider a special case of shifted Killingbeck potential to recover known results.

Study of Davydov–Chaban approach considering shifted Killingbeck potential for any l-state

Relativistic Dirac-attractive radial problem with Yukawa-like tensor interaction via SUSYQM

In this paper, the general procedure for obtaining the distribution for the superstatistics is presented. Besides, the new type of effective Boltzmann factor with non-vanishing rth moments for even...

General distribution function for the superstatistics and new superstatistics with non-vanishing rth moments for even r

A Bohr Hamiltonian, with a potential including a displaced harmonic oscillator plus a Coulomb-like term and a centrifuge term for the \( \beta\)-part and a harmonic oscillator centered around \( \gamma= \frac{\pi}{6}\) for the \( \gamma\)-part, which can be approximately separated, has been solved for the \( \beta\)-part and \( \gamma\)-part. The part related to the collective \( \gamma\)-variable has been chosen in such a way that the model describes the triaxial nuclei. The eigenfunctions and eigenvalues of the energy have been obtained. An analytical expression for the total energy spectra is given.

Bohr Hamiltonian and the energy spectra of the triaxial nuclei

In this paper, the formation process of magnesium hydroxide unit cells, as well as the structural characteristics and growth morphology of magnesium hydroxide, is discussed from the perspective of growth units. The growth process of the hexagonal structure of the magnesium hydroxide is as follows: the growth units are first incorporated into a larger hexagonal dimension unit on the same plane, and then the hexagonal layers connect to each other in the z-axis direction for the hexagonal magnesium hydroxide unit cell. The results of the study show that the model of anion coordination polyhedron growth units may be reasonably deduced by using the unit cell structure and growth mechanism of magnesium hydroxide. After using Raman spectroscopy of the magnesium hydroxide growth solution Raman shift, the growth units of the magnesium hydroxide are shown to be octahedral: [Mg-(OH)6]4-.

https://journals.tubitak.gov.tr/chem/issues/kim-14-38-3/kim-38-3-5-1209-7.pdf

Hassan Hassanabadi

Papers

Study of Davydov–Chaban approach considering shifted Killingbeck potential for any l-state

Relativistic Dirac-attractive radial problem with Yukawa-like tensor interaction via SUSYQM

General distribution function for the superstatistics and new superstatistics with non-vanishing rth moments for even r

Bohr Hamiltonian and the energy spectra of the triaxial nuclei

Crystal growth morphology of magnesium hydroxide