Lecture 2 Flashcards

1
Q

CCDs and CMOS detectors work

A

via the photoelectric effect in a semiconductor

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2
Q

Semiconductors

A

In an isolated atom, the atomic energy levels are well spaced out

in solids, atomic levels form blended bands. the low energy bands are filled by electrons up to the fermi level.

in a semiconductor the last filled level is the ‘valence’ band

the valance and higher energy conduction bands are separated in energy by the band gap

electrons must be able to move between energy levels. so full bands cannot participate

electronic conduction arises when an electron moves from the valence band into a higher energy state.

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3
Q

How can a valence electron gain energy and jump the band gap?

A

Thermally
or from the photoelectric effect

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4
Q

to improve a semiconductors conduction, and help store the charges from the photo-electrons, we use

A

doped semiconductors

  • adding a small amount of a different atom to our semiconductor
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5
Q

p-type

A

fewer valence electrons so extra hole

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6
Q

n-type

A

more valence electrons so extra e-

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7
Q

Silicon (MOS) transistor

A

a thin insulator layer of SiO2 is placed onto the p-type Si and on top of this metal electrode

the positive holes are driven away from the small positive bias voltage near the electrode = depletion region

electrons migrate to near electrode

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8
Q

depletion region

A

is the region where the positive holes are driven away from the small positive bias voltage near the electrode

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9
Q

full well capacity

A

maximum number of electrons that can be held before pixel saturates

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10
Q

CCD readout

A

CCDs are readout by applying sequences of voltages along the columns and down the rows of the CCD, transferring charge from one pixel to the next.

For speed all the columns are shifted at the same time.

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11
Q

Analogue to digital converter:

A

converts voltage to data numbers (DN)

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12
Q

3 phase read out scheme

A

each pixel has 3 electrodes connected in parallel at voltages Φ1, Φ2, Φ3

voltage is varied, allowing charge to migrate but also be kept separate

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13
Q

contributions to CCD data numbers (formula)

A

Xij = Pij + Tij + Eij + Cij

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13
Q

Pij =

A

contributions from pixel charge due to photons from the astronomical source

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14
Q

Tij =

A

contribution from pixel charge due to thermal effects (dark current)

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15
Q

Eij =

A

contribution from readout process

16
Q

Cij =

A

contribution from pixel charge due to cosmic ray hits

17
Q

Thermal noise Tij or dark current arises from

A

thermal energy in the CCD material, leading to lattice vibrations, called phonons

energy of these vibrations can create electron-hole pairs in the absence of illumination

18
Q

the electrons give a DN signal, Tij and carry a

A

statistical fluctuation, ΔTij which varies in time

19
Q

dark frames

A

are exposures with no illumination falling on the CCD

dark frames are exposed for long enough to capture thermal patterns

20
Q

Electronic noise Eij

A

each stage of the photo-electrons to DN conversion can contribute noise

21
Q

electron noise can arise in

A

transfer of charge from pixel to pixel

amplification of readout voltage - need low-noise amplifier

measurement of amplified voltage

22
Q

quantisation noise

A

conversion of the analogue voltage into a digital signal (DN) in the ADC introduces an additional error term

23
Q

Bias frames

A

are exposures of zero duration, without light falling on the CCD, which capture the various sources of Eij (not thermal noise)

24
Q

bias frames are needed to

A

quantify the effect of the ADC offset

25
Q

bias frames provide

A

pixel-to-pixel structure in the electron noise

26
Q

a series of bias frames is acquired and averaged to

A

reduce the SNR on the bias frame values

27
Q

output of a CCD is an

A

analogue signal, time-varying voltage

28
Q

CCD voltage is typically composed

A

of bias voltage and small fluctuations due to the electrons in the potential wells

29
Q

pedestal voltage

ADC offset voltage

A

a small offset voltage is added to the CCD output voltage when the output is less than the reference voltage