Measurement |
as
function of |
for
experiment(s) |
Source:
Fig. from paper |
Theta13
sensitivity (exclusion
limit) |
Experiment (comparison bar plot) |
Different beta beam and neutrino
factory setups |
Fig. 6, hep-ph/0506237 |
MINOS, ICARUS, OPERA |
Fig. 3, hep-ph/0403068 | ||
MINOS+ICARUS+OPERA, Double
Chooz, T2K, NOvA |
Fig. 6, hep-ph/0403068 | ||
Reactor experiments, T2K |
Fig. 11, hep-ph/0303232 | ||
Neutrino factory (two setups),
T2K, T2HK |
Fig. 20, hep-ph/0204352 | ||
L and E (muon) |
Neutrino factory |
Fig. 3, hep-ph/0606119 |
|
Integrated luminosity |
Double Chooz, Triple Chooz |
Fig. 1, hep-ph/0601266 | |
Reactor experiments at L=1.05 km
and L=1.7 km |
Fig. 5, hep-ph/0403068 | ||
MINOS, ICARUS, OPERA |
Fig. 2, hep-ph/0403068 | ||
Reactor experiment |
Figs. 2, 3, hep-ph/0303232 | ||
Time |
Double Chooz, Triple Chooz | Fig. 2, hep-ph/0601266 | |
MINOS, Double Chooz, Triple
Chooz, T2K, NOvA (comparison) |
Fig. 5, hep-ph/0601266 | ||
True dm_atm |
Double Chooz, Triple Chooz | Fig. 3, hep-ph/0601266 | |
MINOS+ICARUS+OPERA, Double Chooz, T2K, NOvA | Fig. 7, hep-ph/0403068 | ||
Reactor-I, T2K |
Fig. 6, hep-ph/0303232 | ||
Neutrino factory program vs. JHF
program |
Fig. 12, hep-ph/0204352 | ||
True dm_sol |
MINOS+ICARUS+OPERA |
Fig. 4, hep-ph/0403068 | |
Reactor-I, T2K | Fig. 6, hep-ph/0303232 | ||
Gamma factor |
Beta beams |
Fig. 2, hep-ph/0506237 | |
L |
Beta beams |
Fig. 3, hep-ph/0506237 | |
Reactor experiments |
Fig. 1, hep-ph/0303232 | ||
L1, L2 (two detectors) |
Neutrino factory |
Fig. 1, hep-ph/0301257 | |
Theta13
discovery |
Time, true deltacp (bands) |
MINOS, Double Chooz, Triple Chooz, T2K, NOvA (comparison) | Fig. 5, hep-ph/0601266 |
MINOS, CNGS, Double Chooz, T2K, NOvA, Reactor-II, NOvA+proton driver, 2nd generation superbeam, neutrino factory | Figs. 4, 5, hep-ex/0509019 | ||
True theta13, true deltacp |
Beta beams, neutrino factories,
T2HK |
Fig. 7, hep-ph/0506237 | |
Theta13
precision |
True theta13 |
Double Chooz, Triple Chooz | Fig. 4, hep-ph/0601266 |
Neutrino factory (impact of matter density uncertainties) |
Fig. 4, hep-ph/0307178 | ||
Reactor experiments, T2K |
Fig. 7, hep-ph/0303232 | ||
Neutrino factory (two versions),
T2K, T2HK |
Fig. 12, hep-ph/0204352 | ||
Max. CP
violation discovery
reach (in theta13) |
L and E (muon) |
Neutrino factory |
Fig. 5, hep-ph/0606119 |
Gamma |
Beta beams |
Fig. 8, hep-ph/0506237 | |
True dm_sol |
T2K (two configurations),
Reactor-II |
Fig. 10, hep-ph/0303232 | |
Any CP
violation discovery |
L and E (muon) | Neutrino factory | Fig. 9, hep-ph/0606119 (large
theta13) |
True theta13, true deltacp (as
fraction of deltacp) |
Neutrino factory |
Fig. 23, hep-ph/0606119 | |
MINOS + Double Chooz + T2K + NOvA + astrophysical source | Fig. 6, hep-ph/0604191 | ||
T2HK, SPL, Beta beam, Neutrino
factory |
Fig. 6, hep-ph/0601266 | ||
Beta beams, neutrino factories, T2HK | Fig. 11, hep-ph/0506237 | ||
True theta13, true deltacp
(direct) |
Neutrino factory (impact of matter density uncertainties) |
Fig. 5, hep-ph/0307178 | |
Neutrino factory, T2HK (impact of matter density uncertainties) |
Fig. 7, hep-ph/0307178 | ||
Neutrino factory, T2HK | Fig. 18, hep-ph/0204352 | ||
Deltacp
precision |
True deltacp (for one theta13) |
MINOS + Double Chooz + T2K + NOvA + astrophysical source | Fig. 8, hep-ph/0604191 |
Neutrino factory, T2HK,
T2K+NOvA+Reactor II |
Fig. 4, hep-ph/0412199 | ||
Neutrino factory |
Figs. 6, 7, hep-ph/0412199 | ||
Various T2K, NOvA, Reactor
combinations |
Fig. 3, hep-ph/0310307 | ||
T2HK |
Fig. 4, hep-ph/0310307 | ||
True theta13 (for one deltacp) |
Neutrino factory, T2HK, T2K+NOvA+Reactor II | Figs. 4, 8, hep-ph/0412199 | |
Neutrino factory |
Figs. 5, 7, hep-ph/0412199 | ||
Neutrino factory (impact of matter density uncertainties) |
Fig. 6, hep-ph/0307178 | ||
True theta13 (for all deltacp) | Neutrino factory, T2HK |
Fig. 19, hep-ph/0204352 | |
Theta13-Deltacp-fit
region |
Fit theta13 and fit deltacp |
Double Chooz + astrophysical
source |
Fig. 3, hep-ph/0604191 |
T2K, NOvA, Double Chooz,
Combination |
Figs. 8, 9, hep-ph/0403068 | ||
Mass
hierarchy discovery reach
(in theta13) for specific deltacp |
L and E (muon) | Neutrino factory | Fig. 6, hep-ph/0606119 |
Gamma |
Beta beams | Fig. 8, hep-ph/0506237 | |
True dm_sol |
T2K, NOvA, Reactor-II |
Fig. 9, hep-ph/0303232 | |
Mass
hierarchy discovery for all
deltacp |
True theta13, true deltacp |
Neutrino factory |
Fig. 23, hep-ph/0606119 |
MINOS + Double Chooz + T2K +
NOvA + astrophysical source |
Fig. 5, hep-ph/0604191 | ||
Beta beams, neutrino factories, T2HK | Fig. 12, hep-ph/0604191 | ||
Mass
hierarchy discovery for
theta13=0 |
L |
T2HK-like superbeam, neutrino
factory |
Figs. 6, 9, hep-ph/0509359 |
True dm_atm, L |
T2HK-like superbeam | Fig. 8, hep-ph/0509359 | |
Comparison:
theta13, mass
hierarchy, and CP violation |
Experiment option, theta13 |
Neutrino factory options |
Fig. 22, hep-ph/0606119 |
Experiment option, deltacp |
Beta beams, neutrino factories, T2HK | Fig. 14, hep-ph/0506237 | |
L, gamma |
Beta beams |
Fig. 9, hep-ph/0506237 | |
L (different baselines) |
Neutrino factory |
Fig. 3, hep-ph/0301257 | |
Precision of
dm_atm |
L and E (muon) |
Neutrino factory | Fig. 7, hep-ph/0606119 |
True theta13 |
Reactor experiments, T2K, NOvA |
Fig. 8, hep-ph/0303232 | |
True dm_atm |
CNGS, MINOS, NOvA, T2K |
Fig. 1, hep-ph/0412133 | |
Theta23-dm_atm-fit
region |
Fit theta23 and fit dm_atm |
Conv. beams, T2K, NOvA, Combined |
Fig. 1, hep-ph/0403068 |
Precision
of theta23 |
True dm_atm | CNGS, MINOS, NOvA, T2K | Fig. 1, hep-ph/0412133 |
Exclusion of
octant degeneracy |
True Theta13 and true theta23 |
MINOS + Double Chooz + T2K + NOvA + astrophysical source | Fig. 11, hep-ph/0604191 |
Deviation
from
max. atm. mixing |
L and E (muon) |
Neutrino factory |
Fig. 8, hep-ph/0606119 |
True theta23, true dm_atm |
Conv. beams, T2K, NOvA, T2HK,
Neutrino factory |
Fig. 1, hep-ph/0404268 | |
Matter
density measurement |
theta13 |
Neutrino factory |
Fig. 3, hep-ph/0502097 |
MSW effect
verification |
True theta13, L |
Neutrino factory |
Figs. 1, 2, hep-ph/0411309 |
Sensitivity
to new physics ... |
... for mass-varying neutrinos |
Reactor experiments |
Fig. 2, hep-ph/0606119 |
... for Hamiltonian-level effects |
Neutrino factory |
Figs. 4, 5, hep-ph/0508175 | |
... for decoherence |
Reactor experiments |
Fig. 3, hep-ph/0502147 |
|
... distinguishing ``damping''
effects |
Neutrino factory |
Fig. 5, hep-ph/0502147 |