Difference between revisions of "Bias Card low noise bias lines noise analysis"

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The low noise detector bias lines in Rev F bias cards are driven by a bipolar DAC (MAX5444AEUB+) whose output is buffered by an opamp in a non-inverting configuration (AD797), and inverted by a second opamp (AD797).  These two signals are then each fed through a series resistance before going to the backplane and MDM connectors.  The noise performance of these bias lines is determined by summing the noise contributions of the DAC output resistance, the feedback resistances in the buffer and the voltage and current noise of the op amp. At high frequencies (ignoring 1/f noise), the total noise can be calculated as:
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The low noise detector bias lines in Rev F bias cards are driven by a bipolar DAC (MAX5444AEUB+) whose output is buffered by an opamp (AD797) in a non-inverting configuration (gain G=2), and inverted by a second opamp (AD797).  These two signals are then each fed through a series resistance before going to the backplane and MDM connectors.  The noise performance of these bias lines is determined by summing the noise contributions of:
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-the input resistance to the op amp: ~6.3k, mostly due to the output resistance of the DAC
 +
-the matched feedback resistances of the buffer, which are internal to the DAC (RFB and INV pins): not listed in the datasheet, but measured as ~12k
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-the voltage noise of the op amp: 0.9 nV/rtHz at 1kHz
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-current noise of the op amp: 2.0 pA/rtHz
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which multiplies both the input resistance to the non-inverting input (~6.3k) and the parallel combination of the feedback resistors at the inverting input (~12k each)
  
<math> v_{nt}\ (1kHz,300K) \ = \ \sqrt { e_n^2 + i_n R_i + i_n (R_{f_1} // R_{f_2}) + 4kTR_i + 4kTR_{f_1}(\frac{R_{f_2}}{R_{f_1} + R_{f_2}})^2 + 4kTR_{f_2} (\frac{R_{f_1}}{R_{f_1} + R_{f_2}})^2 } \ \ \ \ \cong \ \ 45 \ \frac{nV}{\sqrt{Hz}} </math>
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Using these numbers, the total noise at 1 kHz and 300 K can be calculated as:
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<math> v_{nt}\ (1kHz,300K) \ = \ G \sqrt { e_n^2 + i_n R_i + i_n (R_{f_1} // R_{f_2}) + 4kTR_i + 4kTR_{f_1}(\frac{R_{f_2}}{R_{f_1} + R_{f_2}})^2 + 4kTR_{f_2} (\frac{R_{f_1}}{R_{f_1} + R_{f_2}})^2 + 4kT} \ \ \ \ \cong \ \ 45 \ \frac{nV}{\sqrt{Hz}} </math>
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This characterizes the flat high frequency noise spectrum of the positive polarity bias line before the series resistance.  The ~233 ohms of series resistance  The ; however, the detector band of interest is up to only 10 Hz.  In this band, 1/f noise will be important.

Revision as of 13:56, 24 February 2011

The low noise detector bias lines in Rev F bias cards are driven by a bipolar DAC (MAX5444AEUB+) whose output is buffered by an opamp (AD797) in a non-inverting configuration (gain G=2), and inverted by a second opamp (AD797). These two signals are then each fed through a series resistance before going to the backplane and MDM connectors. The noise performance of these bias lines is determined by summing the noise contributions of: -the input resistance to the op amp: ~6.3k, mostly due to the output resistance of the DAC -the matched feedback resistances of the buffer, which are internal to the DAC (RFB and INV pins): not listed in the datasheet, but measured as ~12k -the voltage noise of the op amp: 0.9 nV/rtHz at 1kHz -current noise of the op amp: 2.0 pA/rtHz which multiplies both the input resistance to the non-inverting input (~6.3k) and the parallel combination of the feedback resistors at the inverting input (~12k each)

Using these numbers, the total noise at 1 kHz and 300 K can be calculated as:

<math> v_{nt}\ (1kHz,300K) \ = \ G \sqrt { e_n^2 + i_n R_i + i_n (R_{f_1} // R_{f_2}) + 4kTR_i + 4kTR_{f_1}(\frac{R_{f_2}}{R_{f_1} + R_{f_2}})^2 + 4kTR_{f_2} (\frac{R_{f_1}}{R_{f_1} + R_{f_2}})^2 + 4kT} \ \ \ \ \cong \ \ 45 \ \frac{nV}{\sqrt{Hz}} </math>

This characterizes the flat high frequency noise spectrum of the positive polarity bias line before the series resistance. The ~233 ohms of series resistance The ; however, the detector band of interest is up to only 10 Hz. In this band, 1/f noise will be important.