CCD measures intensity prop. to z-component of C-Poynting vector OR |E-field|^2

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    Ccd Intensity Vector
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SUMMARY

The discussion centers on the intensity measurement in a Charge-Coupled Device (CCD) related to the z-component of the C-Poynting vector versus the square of the electric field's magnitude. It is established that intensity is proportional to the expression I = (1/2 μ0) (E x B*)z, which accounts for both electric and magnetic fields, particularly in non-transverse electromagnetic waves. The relationship between the electric field components and the Poynting vector is clarified, emphasizing that the simpler expression I = (1/2Z0)(|Ex|^2 + |Ey|^2) applies specifically to transverse plane waves. The discussion also highlights the significance of the near field and waveguide scenarios where fields may not be purely transverse.

PREREQUISITES
  • Understanding of electromagnetic theory, specifically the Poynting vector.
  • Familiarity with Charge-Coupled Devices (CCDs) and their operation.
  • Knowledge of electric and magnetic field interactions in wave propagation.
  • Basic grasp of complex conjugation in mathematical expressions.
NEXT STEPS
  • Study the derivation and applications of the Poynting vector in electromagnetic theory.
  • Explore the differences between transverse and non-transverse electromagnetic waves.
  • Learn about the near field effects in electromagnetic wave propagation.
  • Investigate the role of complex conjugation in calculating intensity in various wave scenarios.
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Physicists, electrical engineers, and researchers working with electromagnetic wave theory, CCD technology, and intensity measurement in optical systems.

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intuitively, i would say that in a CCD, the photoelectrons are being "created" only by the electric field of the incident light, so that the intensity is proportional to
|E_x|^2+|E_y|^2,
with the xy-plane coinciding with the CCD plane.
But I have several papers here saying that the intensity is actually proportional to
(\textbf{E}\times\textbf{B}^*)_z.
could someone shed some light on why this should be the case? thanks!
 
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They both basically mean the same thing. The energy flow due to electrodynamic fields in general is described by the Poynting vector S:

S = E x H

For air, the magnetic field H and the magnetic field B are related according to B = μ0 H, leading to:

S =(1/μ0) E x B

The intensity in a certain direction is typically defined as the time-average of the Poynting vector dotted by the direction. For sinusoidal waves, the time-average is found by complex conjugating the magnetic field and multiplying by a half:

I = (<S>t)z =(1/2 μ0) (E x B*)z

If the wave is a transverse plane wave (not always the case), then the electric field and magnetic field are related according to: B= sqrt(μ0ε0) z x E which leads to:

I =(1/2Z0) |E|2

For a transverse wave, there is no z-component to the electric field, only x and y components, so we have finally:

I =(1/2Z0)(|Ex|2 +|Ey|2)

So your last expression is more general, and your first expression only applies to transverse plane waves.
 
thank you for your clear explanation.

forgive my ignorance, but could you point out an example of a non-transversal EM wave?

i'm trying to calculate the intensity on the CCD resulting from a focused light beam. the two formulas give slightly different values, the more general one has a complex component, do you think one should simply take the real part or the modulus?
 
If you are close enough to light sources, the fields are not necessarily transverse. This is called the near field. Also, light in a waveguide (like a fiber optic) is not necessarily transverse. If you are using the expression I =(1/2 μ0) (E x B*)z, then the result should be automatically real-valued only. That is the point of the complex conjugation operation ("*").
 

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