Tunable External Cavity Diode Laser

In summary: So you won't see the atomic spectrum, instead you should see a constant photodiode signal due to the constant wavelength of the laser.
  • #1
cks
165
0
http://optics.ph.unimelb.edu.au/atomopt/publications/littrow_rsi_vol72_p4477_2001.pdf

The picture of the ECDL I explain can be found from the above web site.

The purpose of piezo is to change the cavity length of the diode laser, so that the wavelength can be varied.

From the picture, there are two PZT. One is PZT stack, and the other one is PZT disk.


PZT disk: change the cavity length.

I have one question. I wonder why when I turn on the laser, my photodiode can only detect the signal of the laser only if I turn on the PZT stack?

Thank you.
 
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  • #2
Really just a guess, but looking at the arrangement in the pdf, with the stack off the mirror tilts and the beam alignment would be skewed.
Lasers require the mirrors to be parallel.
 
  • #3
cks said:
I have one question. I wonder why when I turn on the laser, my photodiode can only detect the signal of the laser only if I turn on the PZT stack?

Are you saying the laser is definitely on and produces a laser beam, but the photodiode gives no signal? And the beam (if there is one) is hitting the photodiode?

Or do you mean there really is no laser beam, even though the laser is being powered?

NoTime said:
Really just a guess, but looking at the arrangement in the pdf, with the stack off the mirror tilts and the beam alignment would be skewed.
Lasers require the mirrors to be parallel.

That mirror is not one of the laser cavity mirrors. Note how it is 45 degrees to the beam.

It's the grating that functions as a cavity mirror here. Some wavelength is reflected back to the diode, and that determines the wavelength of the laser. Changing the grating angle changes what wavelength is reflected back to the diode.

Regards,

Mark
 
  • #4
First, thank you for your response.

Here is the link that I uploaded to youtube for easy explanation.


Redbelly98, you're right, the diffraction grating and the mirror are parallel to each oher and lie 45 degrees to the grating mount.

As you can see from the video, the diode output beam hit the diffraction grating. The zeroth order diffracted beam will be diffracted to the mirror and travel to the vapor glass cell. Whereas, the 1st order beam is reflected back to the diode itself.

The absorption spectrum of the atoms are shown on the oscilloscope.

As you can see, the function generator is connected to the PZT stack. The generator gives out a triangle wave of certain voltage to the PZT stack. The PZT stack as mentioned earlier is to tune the wavelength of the laser by rotating the angle of the diffraction grating.

I couldn't explain why the on and off of the funciton generator make the pattern disappear??

Thank you.
 
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  • #5
When you don't have a ramp voltage going to the stack, you are no longer scanning the wavelength. So you won't see the atomic spectrum, instead you should see a constant photodiode signal due to the constant wavelength of the laser.

Can you answer three questions for me (to help me better understand what is happening):

1. When the PZT stack voltage is off, is the photodiode signal zero or non-zero?
2. When the PZT stack voltage is off, is there a beam coming out of the diode that you can see (either visibly or with eg. an IR sensor card)?
3. Was the oscilloscope on AC or DC mode in the video?
 
  • #6
Thank you, I think I understand what you mean. You mean in a single wavelength, it's hardly any absorption. But by varying the wavelength in a small size. there'll be different absorption regarding how closed the wavelength to the energy level difference. So, you can see a pattern.

Am I understanding what you said correctly?

However, to your explanation, I also find it a bit weird. When there's no pattern on the scope(pzt stack off), I still can see a fluorescence line in the vapor cell by using infrared conversion viewer which means absorption occurs as the electrons are jumping down to lower level giving out lights.

Answers to your questions:
1. photodiode diode signal is zero(coz I use AC for oscilloscope)
2. Yes.
3. AC. (So, when I put in DC mode, I can see a shift of the whole horizontal line vertically when PZT stack is off)


Thank you.
 
  • #7
cks said:
Thank you, I think I understand what you mean. You mean in a single wavelength, it's hardly any absorption.

Not quite. I mean the absorption will be a fixed, constant amount.

But by varying the wavelength in a small size. there'll be different absorption regarding how closed the wavelength to the energy level difference. So, you can see a pattern.
Yes. The amount of absorption depends on the wavelength, so:
Vary the wavelength --> vary the absorption signal
Constant wavelength --> constant absorption signal

Am I understanding what you said correctly?
I think so.

However, to your explanation, I also find it a bit weird. When there's no pattern on the scope(pzt stack off), I still can see a fluorescence line in the vapor cell by using infrared conversion viewer which means absorption occurs as the electrons are jumping down to lower level giving out lights.
Okay, that's helpful to know. So the laser is on, and the wavelength is close enough to the absorption peak to produce fluorescence. If you turn the adjustment screw located at the PZT stack (with PZT stack still off), you should see the fluorescence get brighter or dimmer as you turn that screw.

Answers to your questions:
1. photodiode diode signal is zero(coz I use AC for oscilloscope)
2. Yes.
3. AC. (So, when I put in DC mode, I can see a shift of the whole horizontal line vertically when PZT stack is off)

Replies to your answers:
1. No, the photodiode signal is unknown when you measure in AC mode. Use either DC mode, or a voltmeter mode, to measure what the signal is.
2. Good, I had wondered originally if you really meant the laser does not come on, but now I see that it is in fact on.
3. Okay. That means there is a signal from the photodiode, since you see a nonzero voltage when the scope is in DC mode.

Everything seems to work just as it should. If anything is still unclear, feel free to ask.
 

1. What is a tunable external cavity diode laser?

A tunable external cavity diode laser is a type of laser that uses a diode as the gain medium and an external cavity to tune the laser's output wavelength. This allows for a wide range of wavelengths to be produced, making it useful for a variety of scientific and industrial applications.

2. How does a tunable external cavity diode laser work?

The diode laser emits light when an electric current is applied, but the specific wavelength of the light is determined by the properties of the external cavity. The external cavity acts as a wavelength-selective filter, allowing only certain wavelengths to pass through and be amplified by the diode. By changing the length of the external cavity, the wavelength of the laser can be tuned.

3. What are the advantages of using a tunable external cavity diode laser?

One major advantage is its tunability, which allows for a wide range of wavelengths to be produced without the need for different lasers. It also has a compact size and high efficiency, making it ideal for use in various applications such as spectroscopy, material processing, and telecommunications.

4. Are there any limitations to using a tunable external cavity diode laser?

One limitation is that the tuning range may be limited by the properties of the external cavity. Additionally, the output power may be lower compared to other types of lasers, making it less suitable for certain applications that require high power output.

5. What are some common uses for tunable external cavity diode lasers?

Tunable external cavity diode lasers are commonly used in spectroscopy, where the ability to tune the laser's wavelength is crucial for analyzing different types of samples. They are also used in material processing, such as cutting and welding, as well as in telecommunications for optical communication systems.

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