Maptek Vulcan Crack Pes 2016

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.Ofude, Mitsuo; Shimá, Takashi; Yotsuyanagi, Satóshi; Ikeda, Daisuke2017-04-01To assess the predictors of the overall laser energy (TLE) needed during ureteroscopic lithotripsy (URS) making use of the hoImium:yttrium-aluminum-garnét (Ho:YAG) laser for a single ureteral rock. We retrospectively analyzed the information of 93 URS procedures carried out for a solitary ureteral rock in our institution from November 2011 to Sept 2015. We evaluated the organization between TLE and preoperative scientific data, like as age group, sex, entire body mass catalog, and noncontrast computed tomographic findings, including stone laterality, place, maximum diameter, volume, stone attenuation values measured making use of average Hounsfield systems (HUs), and presence of secondary indicators (serious hydronephrosis, tissues rim sign, and perinephric stranding). The just mean maximum stone diameter, quantity, and average HUs had been 9.2 ± 3.8 mm, 283.2 ± 341.4 mm 3, and 863 ± 297, respectively. The just mean TLE and surgical time were 2.93 ± 3.27 kJ and 59.1 ± 28.1 mins, respectively. Optimum stone diameter, volume, average HUs, serious hydronephrosis, and tissues rim indication were significantly correlated with TLE (Spearman'h rho analysis). Stepwise several linear regression evaluation defining stone volume, typical HUs, severe hydronephrosis, and tissues rim sign as explanatory variables showed that rock volume and average HUs were substantial predictors of TLE (standardised coefficients of 0.565 and 0.320, respectively; adjusted L 2 = 0.55, Y = 54.7, P.Rath, Asawari N.; Kundu, S i9000.; Ray, A new.

Maptek Vulcan Crack Pes 2016 Pc Free

K.2018-02-01Laser induced photoionization of atoms displays significant dependence on the selection of polarizations óf lasers. In muIti-step, multi-phóton excitation and following ionization of atoms different polarization combos of the exciting lasers lead to distinctly different ion yields. This fact is exploited in this work to determine total angular momenta óf odd-parity energy ranges of U I lying at ∼ 4 eV from its terrain level making use of resonance ionization laser polarization spectroscopy in time of airline flight bulk spectrometer.

These ranges are filled by two-stép resonant excitation using two pulsed color lasers with preset polarizations of selection implemented by nonresonant ionization by third laser beam. The dependence of ionization produce on specific polarizations of the 1st two lasers is researched experimentally for each level under consideration. This dependence when likened to simulations can make achievable unambiguous task of J angular momenta to these ranges.Walker, H. H.; Heinbockel, J. L.1987-01-01Photovoltaic converters are usually of curiosity for converting laser energy to electrical energy in a space-based laser beam power system. This document explains a model for solar laser converters and the software of this design to a neodymium laser silicon solar converter program.

A parametric research which defines the level of sensitivity of the solar parameters is definitely explained. An optimized siIicon photovoltaic converter offers an effectiveness better than 50 percent for 1000 Watts/sq cm of neodymium laser beam rays.Hayden, Yuiko T.; Guesto-Barnak, Dónna1992-01-01A low-or no-silica, reduced- or no-alkali phosphate cup useful as a laser beam amp in a multiple pass, high energy laser beam system having a high thermal conductivity, K.subwoofer.90.degree. 0.85 W/mK, a reduced coefficient of thermal expansion,.alpha.sub.20.degree.-300.degree. 325.mu.secs at 3 wt.% Nd doping, consisting basically of (on an oxide composition base): wherein Ln.subwoofer.2 O.sub.3 can be the amount of lanthanide oxides;.SIGMA.L.sub.2 O is 0.85 W/mK, a low coefficient of thermal development, alphasub 20-300 G 325 musecs at 3 wt.% Nd doping, consisting basically of (on an oxide composition base): (Mole%) Psub 2Obass speaker 5, (52-72); Alsub 2Osub 3, (0-0-25); ZnO, (0-31); Lisub 2O, (0-5); Ksub 2O, (0-5); Nasub 2O, (0-5); Cssub 2O, (0-5); Rbsub 2O, (0-5); MgO, (0.