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SPIRE Design Description - Research Services

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Draft <strong>SPIRE</strong> <strong>Design</strong> <strong>Description</strong> Document<br />

4.2 RF Filters<br />

The bolometer detectors in the spectrometer and the photometer are sensitive to all frequencies of<br />

electromagnetic radiation. Although the BDA feedhorns act as effective high pass filters, it is essential that<br />

emissions from within the FPU unit be minimised to eliminate spurious sources of signal. The harnesses that<br />

pass from the WE on the SVM to the FPU can act as receiving antennas. The voltages received by the<br />

harnesses outside the cryostat could then possibly retransmit EM radiation within the FPU and corrupt the<br />

signals from the BDA.<br />

To eliminate this possible source of noise on the detector signal, low pass RF filters protect all harnesses<br />

passing into the FPU. Three basic types of harnesses pass into the FPU; (i) bolometer signal wires, (ii)<br />

bolometer bias wires, and (iii) FPU sub-system drive and instrumentation wires (eg. Coil drive current wires,<br />

thermistor readout signals etc.). These three types of harnesses can be identified on the <strong>SPIRE</strong> system<br />

diagram, Figure 3-1. The bolometer signals are filtered within the JFET boxes and will described separately<br />

below in §4.3. The bolometer bias harnesses and the subsystem harnesses are conditioned by sets of filter<br />

boxes.<br />

There are six filter boxes for the subsystems are located on the spectrometer side of the FPU (see Figure<br />

3-5). They have two 37 way MDM socket connectors on the WE side of the box connected to two 37 way<br />

MDM plug connectors on the subsystems side of the box. Each pin on WE side of the box is connected to an<br />

equivalent pin on the detector side via a muRata VFM41R01C222N1C 3-terminal varistor-capacitor EMI<br />

filter. There are therefore 444 individual filters allocated to the subsystems. The filter requirement is that it<br />

rejects all frequencies from 500 MHz to 10 GHz at –60 dB. The filter operates by conducting high frequency<br />

noise signals to ground via the third terminal of the filter. The bode diagram showing the insertion losses for<br />

the filter at room temperature and with a 50Ω source impedance is shown in Figure 4-13.<br />

Figure 4-13 – Insertion losses for the muRata EMI filters.<br />

69

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