feat: data process script
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0397ef71f8
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@ -15,3 +15,4 @@ test/
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# Data
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*.root
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*.data
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data/
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@ -1,7 +1,9 @@
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/control/verbose 1
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/run/verbose 2
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/event/verbose 0
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/tracking/verbose 0
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/run/verbose 1
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/event/verbose 1
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/tracking/verbose 1
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/Gene/PrimaryGA/SetBeamEnergy 1 MeV
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# Initialize kernel
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/run/initialize
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69
integral.cpp
69
integral.cpp
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@ -1,39 +1,72 @@
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#include <TFile.h>
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#include <TString.h>
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#include <TTree.h>
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#include <stdio.h>
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void integral(TString file) {
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int integral(TString file) {
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double e[24];
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int id[24], N[1];
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int sum1, sum2;
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int sum1, sum2, sum3;
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TFile f(file);
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if (f.IsZombie()) {
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printf("cannot open root file\n");
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return;
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}
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TTree* t = (TTree*)f.Get("SimData1");
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if (!t) {
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printf("cannot find tree!\n");
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return;
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}
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t->SetBranchAddress("detE", e);
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t->SetBranchAddress("detId", id);
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t->SetBranchAddress("Ndets", N);
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int n = t->GetEntries();
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// printf("n=%d\n", n);
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int i, j;
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sum1 = sum2 = 0;
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sum1 = sum2 = sum3 = 0;
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for (i = 0; i < n; i++) {
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t->GetEntry(i);
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for (j = 0; j < N[0]; j++) {
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if (e[j] > 0.18 && id[j] < 12) {
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sum1++;
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}
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if (e[j] > 0.18 && id[j] > 11) {
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sum2++;
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}
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if (e[j] > 0.18 && id[j] < 12) sum1++;
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if (e[j] > 0.18 && id[j] > 11) sum2++;
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if (e[j] >= 0.64 && e[j] <= 0.8) sum3++;
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}
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}
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printf("%d,%d,%d,%f\n", sum1 + sum2, sum1, sum2, 1.0 * sum1 / sum2);
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// printf("%d, %d, %d, %d, %f\n", n, sum1 + sum2, sum1, sum2, 1.0 * sum1 / sum2);
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// return sum1 + sum2;
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return sum3;
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}
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void process() {
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double or1[5] = {10, 11, 12, 13, 14};
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double or2[5] = {12.14, 13.35, 14.57, 15.79, 17};
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double or3[5] = {14.28, 15.71, 17.14, 18.57, 20};
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// int energy[8] = {600, 650, 700, 750, 800, 850, 900, 950};
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for (int i = 0; i < 5; i++) {
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TString file =
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TString::Format("data/7/%d/Simulation_RunNo_650kev_70mm_%dmm.root", int(or1[i]), int(or1[i] * 10));
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printf("%d\n", integral(file));
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}
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for (int i = 0; i < 5; i++) {
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TString file =
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TString::Format("data/8.5/%.2f/Simulation_RunNo_650kev_85mm_%dmm.root", or2[i], int(or2[i] * 10));
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printf("%d\n", integral(file));
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}
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for (int i = 0; i < 5; i++) {
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TString file =
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TString::Format("data/10/%.2f/Simulation_RunNo_650kev_100mm_%dmm.root", or3[i], int(or3[i] * 10));
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printf("%d\n", integral(file));
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}
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// for (int i = 0; i < 5; i++) {
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// for (int j = 0; j < 8; j++) {
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// TString file = TString::Format("data/7/%d/Simulation_RunNo_%dkev_70mm_%dmm.root", int(or1[i]), energy[j],
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// int(or1[i] * 10));
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// printf("%d\n", integral(file));
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// }
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// }
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// for (int i = 0; i < 5; i++) {
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// for (int j = 0; j < 8; j++) {
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// TString file = TString::Format("data/8.5/%.2f/Simulation_RunNo_%dkev_85mm_%dmm.root", or2[i], energy[j],
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// int(or2[i] * 10));
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// printf("%d\n", integral(file));
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// }
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// }
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}
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2
run.mac
2
run.mac
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@ -6,4 +6,4 @@
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/run/initialize
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/gun/particle neutron
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/control/loop loop.mac energy 0.1 5 0.1
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/control/loop loop.mac energy 0.5 1 0.05
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Binary file not shown.
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@ -0,0 +1,76 @@
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#include "math.h"
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#include "stdlib.h"
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#include "iostream"
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const double pi = 3.1415926535;
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double mass[4];
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double vbeta, vgamma;
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double t3_cm;
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double t4_cm;
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double p3_cm;
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double p4_cm;
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void SetBeamEnergy(double energy) {
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double umass = 931.494;
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double massHe4 = 4.00260325413 * umass;
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double massNe22 = 21.991385114 * umass;
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double massMg25 = 24.98583697 * umass;
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double massn = 939.56563;
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mass[0] = massHe4;
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mass[1] = massNe22;
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mass[2] = massMg25;
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mass[3] = massn;
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double eb = energy + mass[0];
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double pb2 = energy * energy + 2.0 * energy * mass[0];
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double pb = std::sqrt(pb2);
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double esum = eb + mass[1];
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vbeta = pb / esum;
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vgamma = 1.0 / std::sqrt(1.0 - vbeta * vbeta);
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double e_cm2 = esum * esum - pb2;
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double e_cm = std::sqrt(e_cm2);
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double t_cm = e_cm - mass[2] - mass[3];
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if (t_cm < 0.0) {
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std::cout << "No solution!" << std::endl;
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return;
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}
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double t_cm2 = t_cm * t_cm;
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t3_cm = (t_cm2 + 2.0 * mass[3] * t_cm) / e_cm / 2.0;
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t4_cm = (t_cm2 + 2.0 * mass[2] * t_cm) / e_cm / 2.0;
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double p3_cm2 = t3_cm * t3_cm + 2.0 * t3_cm * mass[2];
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double p4_cm2 = t4_cm * t4_cm + 2.0 * t4_cm * mass[3];
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p3_cm = std::sqrt(p3_cm2);
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p4_cm = std::sqrt(p4_cm2);
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}
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void GeneratePrimaries(double thetacmr) {
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double thetalabr;
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double tg_thetalabr =
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p4_cm * std::sin(thetacmr) /
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(vgamma * (p4_cm * std::cos(thetacmr) + vbeta * std::sqrt(p4_cm * p4_cm + mass[3] * mass[3])));
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if (tg_thetalabr >= 1.0e6)
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thetalabr = pi / 2.0;
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else
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thetalabr = std::atan(tg_thetalabr);
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if (thetalabr < 0.0) thetalabr = pi + thetalabr;
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double p4_cmx = p4_cm * std::sin(thetacmr);
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double p4_cmz = p4_cm * std::cos(thetacmr);
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double p4_labx = p4_cmx;
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double p4_labz = vgamma * (p4_cmz + vbeta * (t4_cm + mass[3]));
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double p4_lab = std::sqrt(p4_labx * p4_labx + p4_labz * p4_labz);
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double e4_lab = sqrt(p4_lab * p4_lab + mass[3] * mass[3]) - mass[3];
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// std::cout << thetalabr << ", " << e4_lab << std::endl;
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std::cout << e4_lab << std::endl;
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}
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int main() {
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SetBeamEnergy(1);
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for (int i = 0; i < 100; i++) GeneratePrimaries(i * pi / 100.0);
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return 0;
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}
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@ -0,0 +1,127 @@
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import numpy as np
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from matplotlib import pyplot as plt
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mu = 931.4940954 # MeV/c^2
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class Particle(object):
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"""Define a Particle
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Parameters
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----------
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A : int
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mass number
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m : float
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mass
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"""
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def __init__(self, A, m) -> None:
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self.A = A
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self.m = m
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class Reaction(object):
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"""A Nuclear Reaction A(a,b)B
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target nuclei (A) is assumed to be quiescent
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Parameters
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----------
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a/A/b/B : Particle
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Particle a, A, b, B
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"""
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def __init__(self, a, A, b, B) -> None:
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self.a: Particle = a
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self.A: Particle = A
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self.b: Particle = b
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self.B: Particle = B
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@property
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def Q(self):
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"""Returns Q value of the reaction"""
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return (self.A.m + self.a.m - self.B.m - self.b.m) * mu
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@property
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def threshold(self):
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"""Returns threshold energy of the reaction"""
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if self.Q < 0:
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return -(self.A.m + self.a.m) / self.A.m * self.Q
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return 0
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def eb(self, theta, ke):
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"""Returns energy of b in the lab frame
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Parameters
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----------
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theta : float
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angle between a and b in the lab frame in rad
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ke : float
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kinetic energy of a in MeV
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"""
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i1 = np.sqrt(self.a.A * self.b.A * ke) / (self.B.A + self.b.A) * np.cos(theta)
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i2 = (self.B.A - self.a.A) / (self.B.A + self.b.A) + (self.a.A * self.b.A) / ((self.B.A + self.b.A) ** 2) * (np.cos(theta) ** 2)
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i3 = self.B.A * self.Q / (self.B.A + self.b.A)
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return (i1 + np.sqrt(i2 * ke + i3)) ** 2
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def eB(self, theta, ke):
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"""Returns energy of B in the lab frame
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Parameters
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----------
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theta : float
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angle between a and b in the lab frame in rad
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ke : float
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kinetic energy of a in MeV
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"""
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eb = self.eb(theta, ke)
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i1 = self.a.A / self.B.A * ke + self.b.A / self.B.A * eb
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i2 = 2 * np.sqrt(self.a.A * self.b.A * ke * eb) / self.B.A
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return i1 - i2 * np.cos(theta)
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neutron = Particle(1, 1.008665)
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proton = Particle(1, 1.007825)
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tritium = Particle(3, 3.016049)
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he_3 = Particle(3, 3.016029)
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he_4 = Particle(4, 4.002603)
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ne_22 = Particle(22, 21.991385)
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mg_25 = Particle(25, 24.985837)
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theta = np.linspace(0, np.pi, 100)
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r1 = Reaction(he_4, ne_22, neutron, mg_25)
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res = r1.eb(theta, 1)
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plt.plot(theta, res)
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plt.title(r"$^{22}$Ne($\alpha$,n)$^{25}$Mg, $T_\alpha$=0.8 MeV")
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plt.ylabel(r"$T_n$ (MeV)")
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plt.xlabel(r"$\theta$ (rad)")
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plt.xticks([0, np.pi / 4, np.pi / 2, np.pi * 3 / 4, np.pi], [r"$0$", r"$\pi/4$", r"$\pi/2$", r"$3\pi/4$", r"$\pi$"])
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plt.xlim(0, np.pi)
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plt.show()
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exit(0)
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energy = np.linspace(np.min(res), np.max(res), 100)
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r2 = Reaction(he_3, neutron, proton, tritium)
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# res = r2.eb(theta, 0.0114)
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# res2 = r2.eB(theta, 0.0114)
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res = r2.eb(np.pi / 4, energy)
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res2 = r2.eB(np.pi / 4, energy)
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fig, ax = plt.subplots()
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ax.plot(energy, res, color="C0")
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ax.set_title(r"$^3$He(n,p)$^3$H, $\theta$=$\pi/4$")
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ax.set_xlabel(r"$T_n$ (MeV)")
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ax.set_ylabel(r"$T_p$ (MeV)")
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ax1 = ax.twinx()
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ax1.plot(energy, res2, color="C1")
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ax1.set_ylabel(r"$T_t$ (MeV)")
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plt.tight_layout()
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plt.show()
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@ -0,0 +1,32 @@
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import numpy as np
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from matplotlib import pyplot as plt
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or1 = [10, 11, 12, 13, 14]
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or2 = [12.14, 13.35, 14.57, 15.79, 17]
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energy = [600, 650, 700, 750, 800, 850, 900, 950]
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markers = ["^", "+", "s", "D", "."]
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data = np.loadtxt("test/eff.txt")
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data = data.reshape(10, 8)
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data = data / 10000
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plt.figure(dpi=400)
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ax = plt.subplot(1, 1, 1)
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for k in range(5):
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ax.scatter(energy, data[k], label="{:d}cm".format(or1[k]), marker=markers[k])
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ax.legend(loc="lower left")
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ax.set_xlabel("Energy [keV]", fontsize=15)
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ax.set_ylabel("Efficiency", fontsize=15)
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# ax = plt.subplot(2, 1, 2)
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# for k in range(5):
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# ax.scatter(energy, data[k + 5], label="{:.2f}cm".format(or2[k]), marker=markers[k])
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# ax.legend(loc="lower left")
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# ax.set_xlabel("Energy [keV]", fontsize=15)
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# ax.set_ylabel("Efficiency", fontsize=15)
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plt.tight_layout()
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plt.subplots_adjust()
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# plt.show()
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plt.savefig("/home/fox/Documents/Thesis/figures/chap3/Fig3.png")
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@ -0,0 +1,80 @@
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5389
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5171
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4988
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4774
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4722
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4599
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4533
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4401
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5726
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5605
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5383
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5255
|
||||
5089
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5022
|
||||
4959
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4824
|
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5880
|
||||
5750
|
||||
5613
|
||||
5496
|
||||
5341
|
||||
5233
|
||||
5190
|
||||
5094
|
||||
5885
|
||||
5789
|
||||
5669
|
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5515
|
||||
5480
|
||||
5345
|
||||
5317
|
||||
5121
|
||||
5751
|
||||
5649
|
||||
5455
|
||||
5535
|
||||
5436
|
||||
5266
|
||||
5141
|
||||
5253
|
||||
5766
|
||||
5669
|
||||
5512
|
||||
5378
|
||||
5405
|
||||
5283
|
||||
5127
|
||||
5085
|
||||
5819
|
||||
5720
|
||||
5632
|
||||
5544
|
||||
5472
|
||||
5485
|
||||
5456
|
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5162
|
||||
5650
|
||||
5642
|
||||
5507
|
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5456
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5437
|
||||
5366
|
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5368
|
||||
5361
|
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5567
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5492
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5435
|
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5347
|
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5350
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5248
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5275
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5182
|
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5412
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5353
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5310
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5181
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5219
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5121
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5061
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5055
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@ -0,0 +1,24 @@
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import numpy as np
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from matplotlib import pyplot as plt
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or1 = [10, 11, 12, 13, 14]
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markers = ["^", "+", "s", "D", "."]
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data = np.loadtxt("test/eff2.txt")
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data = data.reshape(3, 5)
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data = data / 10000
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fig = plt.figure(dpi=400)
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ax = plt.subplot(1, 1, 1)
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for k in range(5):
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ax.scatter([7, 8.5, 10], data[:, k], label=r"$R_o/R_i$ = {:.2f}".format(or1[k] / 7), marker=markers[k])
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ax.legend(loc="lower left")
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ax.set_xlabel(r"$R_i$ [cm]", fontsize=15)
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ax.set_ylabel("Efficiency", fontsize=15)
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ax.set_xticks([7, 8.5, 10])
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plt.tight_layout()
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plt.subplots_adjust()
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# plt.show()
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||||
plt.savefig("/home/fox/Documents/Thesis/figures/chap3/Fig5.png")
|
||||
|
|
@ -0,0 +1,15 @@
|
|||
5171
|
||||
5605
|
||||
5750
|
||||
5789
|
||||
5649
|
||||
5669
|
||||
5720
|
||||
5642
|
||||
5492
|
||||
5353
|
||||
5165
|
||||
5030
|
||||
4957
|
||||
4831
|
||||
4642
|
||||
|
|
@ -0,0 +1,24 @@
|
|||
import numpy as np
|
||||
from matplotlib import pyplot as plt
|
||||
|
||||
or1 = [10, 11, 12, 13, 14]
|
||||
markers = ["^", "+", "s", "D", "."]
|
||||
|
||||
data = np.loadtxt("test/inner.txt")
|
||||
data = data.reshape(3, 5)
|
||||
data = data / 10000
|
||||
|
||||
fig = plt.figure(dpi=400)
|
||||
|
||||
ax = plt.subplot(1, 1, 1)
|
||||
for k in range(5):
|
||||
ax.scatter([7, 8.5, 10], data[:, k], label=r"$R_o/R_i$ = {:.2f}".format(or1[k] / 7), marker=markers[k])
|
||||
ax.legend(loc="lower right")
|
||||
ax.set_xlabel(r"$R_i$ [cm]", fontsize=15)
|
||||
ax.set_ylabel("Efficiency", fontsize=15)
|
||||
ax.set_xticks([7, 8.5, 10])
|
||||
|
||||
plt.tight_layout()
|
||||
plt.subplots_adjust()
|
||||
# plt.show()
|
||||
plt.savefig("/home/fox/Documents/Thesis/figures/chap3/Fig6(a).png")
|
||||
|
|
@ -0,0 +1,21 @@
|
|||
395.00000, 0.00000
|
||||
400.00000, 0.00926
|
||||
403.19005, 0.03801
|
||||
408.51147, 0.19876
|
||||
410.83959, 0.30444
|
||||
412.75197, 0.40119
|
||||
418.82171, 0.79712
|
||||
421.48241, 0.93703
|
||||
422.81277, 0.97870
|
||||
425.00000, 1.00000
|
||||
427.63530, 0.98168
|
||||
433.37245, 0.89833
|
||||
440.10736, 0.74651
|
||||
446.75913, 0.60064
|
||||
460.06266, 0.43394
|
||||
465.71666, 0.37440
|
||||
472.45158, 0.26426
|
||||
480.10111, 0.17197
|
||||
490.16190, 0.10053
|
||||
499.97326, 0.05885
|
||||
515.00000, 0.00000
|
||||
|
|
@ -0,0 +1,15 @@
|
|||
2295
|
||||
2811
|
||||
3105
|
||||
3346
|
||||
3515
|
||||
3543
|
||||
3887
|
||||
4070
|
||||
4253
|
||||
4331
|
||||
3835
|
||||
3960
|
||||
4153
|
||||
4236
|
||||
4213
|
||||
|
|
@ -0,0 +1,16 @@
|
|||
import numpy as np
|
||||
|
||||
data = np.loadtxt("ej-200.txt", delimiter=",")
|
||||
|
||||
c = 299792458
|
||||
h = 6.62606957 * 1e-34
|
||||
hc = h * c / (1.6 * 1e-19)
|
||||
|
||||
L = len(data)
|
||||
for k in range(L):
|
||||
print(str(round(hc * 1e9 / data[L - k - 1][0], 3)) + " * eV", end=", ")
|
||||
print()
|
||||
|
||||
for k in range(L):
|
||||
print("{:.5f}".format(round(data[L - k - 1][1], 5)), end=", ")
|
||||
print()
|
||||
|
|
@ -0,0 +1,15 @@
|
|||
2876
|
||||
2794
|
||||
2645
|
||||
2443
|
||||
2134
|
||||
2126
|
||||
1833
|
||||
1572
|
||||
1239
|
||||
1022
|
||||
1330
|
||||
1070
|
||||
804
|
||||
595
|
||||
429
|
||||
|
|
@ -0,0 +1,27 @@
|
|||
import numpy as np
|
||||
from matplotlib import pyplot as plt
|
||||
|
||||
or1 = [10, 11, 12, 13, 14]
|
||||
or2 = [12.14, 13.35, 14.57, 15.79, 17]
|
||||
energy = [600, 650, 700, 750, 800, 850, 900, 950]
|
||||
markers = ["^", "+", "s", "D", "."]
|
||||
|
||||
data = np.loadtxt("test/eff.txt")
|
||||
data = data.reshape(10, 8)
|
||||
|
||||
roi = np.loadtxt("test/roi.txt")
|
||||
roi = roi.reshape(10, 8)
|
||||
roi = 1 - roi / data
|
||||
|
||||
plt.figure(dpi=400)
|
||||
|
||||
for k in range(5):
|
||||
plt.scatter(energy, roi[k], label="{:d}cm".format(or1[k]), marker=markers[k])
|
||||
plt.xlabel("Energy [keV]", fontsize=15)
|
||||
plt.ylabel(r"Energy Leakage Rate $\epsilon$", fontsize=15)
|
||||
plt.legend(loc="lower left")
|
||||
|
||||
plt.tight_layout()
|
||||
plt.subplots_adjust()
|
||||
# plt.show()
|
||||
plt.savefig("/home/fox/Documents/Thesis/figures/chap3/Fig7(a).png")
|
||||
|
|
@ -0,0 +1,80 @@
|
|||
3973
|
||||
3798
|
||||
3656
|
||||
3505
|
||||
3442
|
||||
3391
|
||||
3363
|
||||
3277
|
||||
4219
|
||||
4083
|
||||
3952
|
||||
3875
|
||||
3694
|
||||
3634
|
||||
3680
|
||||
3532
|
||||
4233
|
||||
4283
|
||||
4186
|
||||
4057
|
||||
3921
|
||||
3818
|
||||
3758
|
||||
3745
|
||||
4342
|
||||
4214
|
||||
4178
|
||||
4024
|
||||
3992
|
||||
3954
|
||||
3888
|
||||
3721
|
||||
4202
|
||||
4161
|
||||
4027
|
||||
4012
|
||||
3971
|
||||
3855
|
||||
3760
|
||||
3819
|
||||
4252
|
||||
4194
|
||||
4073
|
||||
3957
|
||||
3945
|
||||
3873
|
||||
3761
|
||||
3638
|
||||
4296
|
||||
4125
|
||||
4112
|
||||
4117
|
||||
4037
|
||||
3986
|
||||
3951
|
||||
3748
|
||||
4144
|
||||
4138
|
||||
4041
|
||||
4001
|
||||
3965
|
||||
3924
|
||||
3951
|
||||
3880
|
||||
4067
|
||||
3990
|
||||
3938
|
||||
3902
|
||||
3933
|
||||
3812
|
||||
3806
|
||||
3772
|
||||
3922
|
||||
3903
|
||||
3913
|
||||
3755
|
||||
3813
|
||||
3772
|
||||
3612
|
||||
3724
|
||||
|
|
@ -0,0 +1,28 @@
|
|||
import numpy as np
|
||||
from matplotlib import pyplot as plt
|
||||
|
||||
or1 = [10, 11, 12, 13, 14]
|
||||
or2 = [12.14, 13.35, 14.57, 15.79, 17]
|
||||
energy = [600, 650, 700, 750, 800, 850, 900, 950]
|
||||
markers = ["^", "+", "s", "D", "."]
|
||||
|
||||
data = np.loadtxt("test/eff2.txt")
|
||||
data = data.reshape(3, 5)
|
||||
|
||||
roi = np.loadtxt("test/roi2.txt")
|
||||
roi = roi.reshape(3, 5)
|
||||
roi = 1 - roi / data
|
||||
|
||||
plt.figure(dpi=400)
|
||||
|
||||
for k in range(5):
|
||||
plt.scatter([7, 8.5, 10], roi[:, k], label=r"$R_o/R_i$ = {:.2f}".format(or1[k] / 7), marker=markers[k])
|
||||
plt.xlabel(r"$R_i$ [cm]", fontsize=15)
|
||||
plt.xticks([7, 8.5, 10])
|
||||
plt.ylabel(r"Energy Leakage Rate $\epsilon$", fontsize=15)
|
||||
plt.legend(loc="lower right")
|
||||
|
||||
plt.tight_layout()
|
||||
plt.subplots_adjust()
|
||||
# plt.show()
|
||||
plt.savefig("/home/fox/Documents/Thesis/figures/chap3/Fig7(b).png")
|
||||
|
|
@ -0,0 +1,15 @@
|
|||
3798
|
||||
4083
|
||||
4283
|
||||
4214
|
||||
4161
|
||||
4194
|
||||
4125
|
||||
4138
|
||||
3990
|
||||
3903
|
||||
3745
|
||||
3638
|
||||
3624
|
||||
3532
|
||||
3410
|
||||
Loading…
Reference in New Issue