source: GLBFrejus/HEAD/data/SPL-PRD.glb@ 689

Last change on this file since 689 was 153, checked in by campagne, 19 years ago

add fluxes for 4.5GeV option
File size: 5.0 KB
RevLine 
[153]1%!GLoBES
2/*
3 * If you modify this file you have to rename it.
4 *
5 *
6 %This file has been used in the following references
7
8@Article{Campagne:2005nm,
9 author = "Campagne, J. -E.",
10 title = "The SPL-Fr\'{e}jus physics potential",
11 journal = "Nuclear Physics B (Proceedings Supplement)",
12 volume = "",
13 year = "2005",
14 eprint = "hep-ex/0510029",
15 SLACcitation = "%%CITATION = HEP-EX 0510029;%%"
16}
17
18@Article{Mezzetto:2005,
19 author = "Mezzetto, Mauro",
20 title = "Beta beams",
21 journal = "Journal of Physics: Conference Series",
22 volume = "",
23 year = "2005",
24 pages = "",
25 eprint = "",
26 SLACcitation = ""
27}
28
29@Article{Schwetz:2005,
30 author = "Schwetz, Thomas",
31 title = "Resolving parameter degeneracies with atmospheric neutrinos",
32 journal = "Nuclear Physics B (Proceedings Supplement)",
33 volume = "",
34 year = "2005",
35 pages = "",
36 eprint = "",
37 SLACcitation = ""
38}
39
40/* Version of the File: 1.0 */
41/* Original author: M. Mezzetto */
42/* History: 03/06/05 first version M.M*/
43/* 11/10/05 Tagging for ISS comparison J.E.C*/
44
45
46$version="1.8.1"
47
48/* Beam data */
49/* @time has units `years' */
50/* Norm must contain Len**2 times 6E32 time 1E-38 divided flux bin width (GeV) divided 5.2 */
51
52flux(#SPLplus)<
53 @flux_file = "../data/SPLGLoBESPiPlus.dat"
54 @time = 2
55 @norm = 0.975E-6
56>
57
58flux(#SPLminus)<
59 @flux_file = "../data/SPLGLoBESPiMinus.dat"
60 @time = 8
61 @norm = 0.975E-6
62>
63
64$target_mass = 440
65
66$sampling_points = 30
67$sampling_min = 0.
68$sampling_max = 1.2
69$bins = 5
70$emin = 0.08
71$emax = 1.08
72
73
74/* Baseline */
75
76$profiletype = 3
77$densitytab = {2.7}
78$lengthtab = {130.0}
79
80/* Technical information */
81
82$filter_state = 0
83$filter_value = 1000000
84
85/* Energy Resolution */
86
87/* The same as SK: a constant term corresponding to Fermi motion */
88energy(#ERES)<
89 @type = 1
90 @sigma_e = {0.0,0.0,0.085}
91>
92
93
94/* Cross sections */
95
96cross(#CC)<
97 @cross_file = "../data/LipariXCCGLoBES.dat"
98>
99
100cross(#NC)<
101 @cross_file = "../data/XNC.dat"
102>
103
104/* Channels */
105channel(#numu_non_osci)<
106 @channel = #SPLplus: +: NOSC_m: muon: #CC: #ERES
107>
108
109channel(#nue_app)<
110 @channel = #SPLplus: +: m: e: #CC: #ERES
111>
112
113channel(#nue_bar_app)<
114 @channel = #SPLminus: -: m: e: #CC: #ERES
115>
116
117channel(#numu_disa)<
118 @channel = #SPLplus: +: m: m: #CC: #ERES
119>
120
121channel(#numu_bar_disa)<
122 @channel = #SPLminus: -: m: m: #CC: #ERES
123>
124
125channel(#NC_bckg_plus)<
126 @channel = #SPLplus: +: NOSC_m: NOSC_m: #NC: #ERES
127>
128
129channel(#NC_bckg_minus)<
130 @channel = #SPLminus: -: NOSC_m: NOSC_m: #NC: #ERES
131>
132
133channel(#nue_Beam)<
134 @channel = #SPLplus: +: e: e: #CC: #ERES
135>
136
137channel(#nue_bar_Beam)<
138 @channel = #SPLminus: -: e: e: #CC: #ERES
139>
140
141channel(#nue_in_nubare)<
142 @channel = #SPLminus: +: e: e: #CC: #ERES
143>
144
145channel(#nubare_in_nue)<
146 @channel = #SPLplus: -: e: e: #CC: #ERES
147>
148channel(#numu_disa_signal)<
149 @channel = #SPLplus: +: m: m: #CC: #ERES
150 @pre_smearing_efficiencies={0., 0., 0., 0., 0., 0.16986, 0.5624, 0.715028, 0.77302, 0.86964, 0.92296, 0.95628, 0.9996, 0.98294, 0.96628, 0.94296, 0.9263, 0.89964, 0.88298, 0.85966, 0.843, 0.82634, 0.80968, 0.78302, 0.76636, 0.76636, 0.76636, 0.76636, 0.76636, 0.76636}
151
152>
153
154channel(#numu_bar_disa_signal)<
155 @channel = #SPLminus: -: m: m: #CC: #ERES
156 @pre_smearing_efficiencies={0., 0., 0., 0., 0., 0.16986, 0.5624, 0.715028, 0.77302, 0.86964, 0.92296, 0.95628, 0.9996, 0.98294, 0.96628, 0.94296, 0.9263, 0.89964, 0.88298, 0.85966, 0.843, 0.82634, 0.80968, 0.78302, 0.76636, 0.76636, 0.76636, 0.76636, 0.76636, 0.76636}
157>
158
159/* Rules */
160
161
162rule(#NU_E_app)<
163 @signal = 0.707@#nue_app
164 @signalerror = 0.02 : 0.0001
165 @background = 0.00054@#numu_disa : 0.707@#nue_Beam : 0.677@#nubare_in_nue : 0.00065@#NC_bckg_plus
166 @backgrounderror = 0.02 : 0.0001
167 @backgroundcenter = 1.0 : 0.0
168 @errordim_sys_on = 0
169 @errordim_sys_off = 2
170 @energy_window = 0.1 : 1.
171>
172
173
174rule(#NU_E_BAR_app)<
175 @signal = 0.677@#nue_bar_app
176 @signalerror = 0.02 : 0.0001
177 @background = 0.00054@#numu_bar_disa : 0.707@#nue_in_nubare : 0.677@#nue_bar_Beam : 0.0025@#NC_bckg_minus
178 @backgrounderror = 0.02 : 0.0001
179 @backgroundcenter = 1.0 : 0.0
180 @errordim_sys_on = 0
181 @errordim_sys_off = 2
182 @energy_window = 0.1 : 1.
183>
184
185rule(#NUMU_DISA)<
186 @signal = 1@#numu_disa_signal
187 @signalerror = 0.02 : 0.0001
188 @background = 0.000043@#numu_disa
189 @backgrounderror = 0.02 : 0.0001
190 @backgroundcenter = 1.0 : 0.0
191 @errordim_sys_on = 0
192 @errordim_sys_off = 2
193 @energy_window = 0.1 : 1.
194>
195
196rule(#NUMUBAR_DISA)<
197 @signal = 1@#numu_bar_disa_signal
198 @signalerror = 0.02 : 0.0001
199 @background = 0.000043@#numu_bar_disa
200 @backgrounderror = 0.02 : 0.0001
201 @backgroundcenter = 1.0 : 0.0
202 @errordim_sys_on = 0
203 @errordim_sys_off = 2
204 @energy_window = 0.1 : 1.
205>
206/**********************END********************************************************************************************************************************************************************************************************************************************************************/
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