| Figure 1:
Allowable parameter spaces for |
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| Figure 2:
The left-hand panel from [143] shows the joint constraints on the baryonic matter and dark matter densities, together with the allowed band of baryonic density from BBN models. The right-hand panel from [41] shows the joint constraints on |
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| Figure 3:
Possible scale-lengths where different types of dark matter might be present, based on a similar representation which appeared in [30]. |
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Figure 4:
High-resolution N-body simulation of a galactic dark matter halo [89]. |
| Figure 5:
The rotation curve of the Milky Way. In the left-hand panel are the measured rotation speeds given by the average values from a number of measurements on different objects [50]. The right hand panel shows the various mass components that combine together to reproduce the observed curve between 5 and 25 kpc [72]. The dotted lines are the bulge and disk contributions, and the short-dashed curve is the dark matter contribution. The solid curve shows the combined effect of all three, and this is compared to the long-dashed curve which approximates the measured data in the left-hand panel below 25 kpc. |
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Figure 6:
Total neutralino elastic scattering cross-section normalised to one nucleon for a range of neutralino models within MSSM and mSUGRA, taken from [79]. The pink area corresponds to a neutralino in a dominantly bino state, the green bounded area is dominantly higgsino. The cross-section includes both spin-independent and spin-dependent contributions, and in general the spin-dependent part is likely to be larger. |
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Figure 7:
Background energy spectra for two Ge detectors of the PNL/USC/Zaragoza group taken from [28] (a – upper panel). Coherent cross-section upper limits from Ge detectors taken from [2] (b – lower panel). |
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Figure 8:
Background rate from 428.1 days of data binned in 10-minute intervals and folded to look for daily modulation [2] (a – upper panel). Results of an annual modulation search using |
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Figure 9:
Differential pulse shapes from NaI for various radiation types. There is a clear difference between the functional form for high |
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Figure 10:
Differential time constant distributions from the UK NaI experiment [105, 118] showing the measured background (solid line + data points), and neutron and |
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Figure 11:
The two-phase xenon test chamber used by Wang [35]. |
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Figure 12:
Relative signal amplitudes for |
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Figure 13:
Relative figures of merit for the discrimination potential in NaI, cooled NaI and two-phase liquid xenon [117]. In this plot a lower figure of merit implies proportionately better performance. |
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Figure 14:
Latest published upper limits on (a – upper panel) coherent and (b – lower panel) axial coupled WIMP-nucleon cross-sections adapted from [23]. |
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Figure 15:
The upper panel shows the region of coherent cross-section parameter space consistent with the DAMA NaI annual modulation results [16]. The four curves show the results from each individual year of the four year period shown in Figure 8. The lower panel shows a scatter plot of possible MSSM models which populate the region defined by the first two years of data from [22]. Open circles are cosmologically interesting. |
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Figure 16:
The upper panel shows the current results on the allowed coherent cross-section parameter space. The plot is from [14] and shows the CDMS 3 |
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Figure 17:
Expected progress in covering MSSM parameter space from both indirect and direct search techniques over the next several years [49]. |
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