Highlights, 2016
 
The WIMP cross-section σ χ−n
September 11, 2016
Picture: The WIMP cross-section σ χ−n
The WIMP cross-section σ χ−n
Upper limit (90% C.L.) on the WIMP cross-section σ χ−n obtained with a small data set taken during DAMIC100 R&D phase (red line). Even if limited by the exposure and the level of radiogenic background — both to significantly improve in the upcoming DAMIC100 — these results demonstrate DAMIC’s sensitivity in the low-mass WIMP region (<10 GeV c−2), where the experiment is particularly competitive thanks to its low energy threshold.Learn more >>

 
Measurement of the nuclear recoil ionization efficiency in Silicon
September 9, 2016
Picture: Measurement of the nuclear recoil ionization efficiency in Silicon
Measurement of the nuclear recoil ionization efficiency in Silicon
The energy deposited into ionization, Ee, as a function of the nucleus recoil energy, Er. These are the first measurements of sub-keV nuclear recoils in Silicon.Learn more >>

 
DAMIC installation at SNOLAB
September 7, 2016
Picture: DAMIC installation at SNOLAB
DAMIC installation at SNOLAB
The copper vacuum vessel housing the CCDs is inserted in the lead shield.

 
The DAMIC at SNOLAB lead shielding
September 5, 2016
Picture: The DAMIC at SNOLAB lead shielding
The DAMIC at SNOLAB lead shielding
The innermost layer is made of ancient lead recovered from a sunken Spanish galleon and a Roman ship.

 
The copper box hosting the CCDs
September 3, 2016
Picture: The copper box hosting the CCDs
The copper box hosting the CCDs
The copper box hosting the CCDs, top lead shield and in-vacuum electronics being inserted in the copper vacuum vessel.

 
DAMIC installation at SNOLAB
September 1, 2016
Picture: DAMIC installation at SNOLAB
DAMIC installation at SNOLAB
A packaged CCD being inserted in the copper box. Above the box is a lead cylinder shielding the CCDs from radiogenic backgrounds. DAMIC is taking data at SNOLAB with 7 CCDs for a total mass of 40 g.

 
An alpha and a beta particle originating from the same location in the CCD
August 31, 2016
Picture: An alpha and a beta particle originating from the same location in the CCD
An alpha and a beta particle originating from the same location in the CCD
An alpha and a beta particle originating from the same location in the CCD, consistent with a nuclide from the Th chain undergoing subsequent decays. The excellent spatial resolution of the CCD provides a unique handle in the understanding of the radiogenic background.

 
Particle identification by a DAMIC CCD
August 29, 2016
Picture: Particle identification by a DAMIC CCD
Particle identification by a DAMIC CCD
A muon (straight track); an alpha particle (round blob); an electron (worm-like track) and low-energy particles (electrons from X rays or nuclear recoils).

 
DAMIC100 CCD
August 27, 2016
Picture: DAMIC100 CCD
DAMIC100 CCD
A DAMIC100 CCD with a 6 cm x 6 cm active area (16 Mpixels) and a record thickness of 675 μm. Material selection and surface cleaning of the copper support is optimized for low radiogenic background. The kapton cable services the CCD with clocks, bias voltages and signals.