scholarly journals Application of He Chengtian’s interpolation to Bethe equation

2009 ◽  
Vol 58 (11-12) ◽  
pp. 2427-2430 ◽  
Author(s):  
Ji-Huan He
Keyword(s):  
2019 ◽  
Vol 9 (1) ◽  
Author(s):  
D. M. Martinez ◽  
M. Rahmani ◽  
C. Burbadge ◽  
C. Hoehr

AbstractWhile the dose deposition of charged hadrons has received much attention over the last decades starting in 1930 with the publication of the Bethe equation, there are still practical obstacles in implementing it in fields like radiotherapy and isotope production on cyclotrons. This is especially true if the target material consists of non-homogeneous materials, either consisting of a mixture of different elements or experiencing phase changes during irradiation. While Monte-Carlo methods have had great success in describing these more difficult target materials, they come at a computational cost, especially if the problem is time-dependent. This can greatly hinder optimal advancement in therapy and isotope targetry. Here, a regular perturbation method is used to solve the Bethe equation in the limit of small relativistic effects. Particular focus is given to incident energy level relevant to radionuclide production and radiotherapy applications, i.e. 10–200 MeV. We present a series solution for the range and dose distribution in terms of elementary functions, as opposed to special functions which will aid in uptake by practitioners.


2002 ◽  
Vol 16 (14n15) ◽  
pp. 2097-2106
Author(s):  
SHAO-SHIUNG LIN ◽  
SHI-SHYR ROAN

In this report, we study the algebraic geometry aspect of Hofstadter type models through the algebraic Bethe equation. In the diagonalization problem of certain Hofstadter type Hamiltonians, the Bethe equation is constructed by using the Baxter vectors on a high genus spectral curve. When the spectral variables lie on rational curves, we obtain the complete and explicit solutions of the polynomial Bethe equation; the relation with the Bethe ansatz of polynomial roots is discussed. Certain algebraic geometry properties of Bethe equation on the high genus algebraic curves are discussed in cooperation with the consideration of the physical model.


1995 ◽  
Vol 10 (06) ◽  
pp. 875-894 ◽  
Author(s):  
SRINANDAN DASMAHAPATRA

We outline the relationship between the thermodynamic densities and quasiparticle descriptions of spectra of RSOS models with an underlying Bethe equation. We use this to prove completeness of states in some cases and then give an algorithm for the construction of branching functions of their emergent conformal field theories. Starting from the Bethe equations of Dn type, we discuss some aspects of the Zn lattice models.


Author(s):  
Nestor J. Zaluzec

There has during the last few years been a renewed interest in the calculation of ionization cross-sections for use in AEM-based x-ray analysis, due to the fact that modern AEM's can operate up to accelerating potentials of 400 kV. In this regime relativistic effects are considerable and the extrapolation of the “accepted” microprobe-based formulae to these levels is questionable and the relativistic Bethe equation is the most appropriate formulation.


1967 ◽  
Vol 37 (2) ◽  
pp. 372-397 ◽  
Author(s):  
Hitoshi Ito ◽  
Masayoshi Mizouchi ◽  
Toshiyuki Murota ◽  
Tadao Nakano ◽  
MatuTarow Noda ◽  
...  

Author(s):  
R.A. Ploc

Three aberrations contribute to the loss of image resolution in the transmission electron microscope; spherical (SA=Csα3), chromatic (CA=Ccα△VV-1) and diffraction (DA=O.61ƛα-1). For high voltage incident electrons and thin materials most microscopists assume resolution is controlled by spherical and diffraction aberrations. We shall discuss whether equating the SA and DA to derive an optimum aperture size (related to αo) and resolution limit (1) is a valid procedure.To determine △V for a given material requires the use of either the Bethe or Landau equations. The Landau formula can be used to give the width of the energy spectrum and the Bethe equation, the mean energy loss after the incident electrons pass through the foil. Since the former is the most probable quantity contributing to CA, Figures 1 and 2 are based on the use of the Landau equation. Zirconium of thickness, t, will be considered for the accelerating voltages 105 and 106 eV.


Author(s):  
C. J. Powell

Values of cross sections for ionization of inner-shell electrons by electron impact are required for electron probe microanalysis, Auger-electron spectroscopy, and electron energy-loss spectroscopy. The present author has reviewed measurements and calculations of inner-shell ionization cross sections. This paper is an update and summary of these previous reviews.It is convenient to start with the Bethe equation for inner-shell ionization cross sections which is frequently used (and misused) in x-ray microanalysis:(1)where σnℓ is the cross section for ionization of the nℓ shell with binding energy Enℓ by incident electrons of energy E. The terms bnℓ and cnℓ are the Bethe parameters discussed further below. It has been assumed in the derivation of Eq. (1) that E ≫ Enℓ ; this requirement will also be discussed. Finally, it has been assumed here that E is low enough (≲50 keV) so that a relativistic correction is unnecessary.The extent to which a given set of measured or calculated cross-section data is consistent with Eq. (1) can be determined from a Fano plot in which σnℓE is plotted versus ℓnE; if such a plot is linear, Eq. (1) is consistent with the data and values of the Bethe parameters can be easily derived.


Sign in / Sign up

Export Citation Format

Share Document