User:Pranav Rathi/Notebook/OT/2010/05/12 - Revision history

Pranav Rathi: Replacing page with '/Characterization of AOM module Category:Random'

Pranav Rathi — Thu, 15 Nov 2012 18:01:08 GMT

Replacing page with '/Characterization of AOM module Category:Random'

←Older revision		Revision as of 18:01, 15 November 2012
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	[[/Characterization of AOM module]]		[[/Characterization of AOM module]]
-	~~==AOM Characterization==~~
-	~~===Introduction:===~~
-	The motive of doing this is to attend enough information, to use AOM as power modulator for the tweezer. AOM (Gooch & Housego R23080-2-1.06-LTD; 138252) operates in CW and normal mode. We use 1st order diffracted beam. First CW mode operation is characterized, to know the usable power (of the diffracted beam) Vs ascending input laser power. Second normal mode operation is characterized: Computer controlled ascending input voltage for RF signal power Vs usable power of the diffracted beam, at several input laser powers. The laser temperature is kept constant at 62F.

-	~~===Setup:===~~	+	[[Category:Random]]
-	~~Relatively simple setup ThorLabs power meter is place infront of the diffracted beam from AOM. An aperture is used infront of the power meter to keep off all the stray beams.~~	+
-		+
-	~~[[Image:AOM_char-setup.JPG]]~~	+
-		+
-	~~===CW mode operation characterization:===~~	+
-	~~The AOM is operating in CW mode. Data is recorded; laser power (.25W to 4W in .25W increments) Vs 1st order beam power. This 1st order beam power is the usable power for tweezer.~~	+
-	~~The data is presented below:~~	+
-	~~{{ShowGoogleExcel\|id=0ApjWjFYiQdkfdHZ1VTdkaGFGbDFnSmtpUHJGdzR5aWc\|width=800\|height=500}}~~	+
-	~~====Result:====~~	+
-	'''''The relationship is linear. So the AOM gives output power in 1st order diffracted beam, of average around 70% of the input power (in CW mode).''''' This help us calculating the usable power of any input power without measuring; for example if I set the laser on .10W, then the usable power at the tweezer is 70% of it, which is .07W or 70mW.The maximum usable power for the tweezer is 2.66W. If we want to stay in the single mode operation regime, it is 1.4W (at room temperature). When the laser is cooled down to 60F, it is stretched to 1.9W (2.75W input).	+
-		+
-	~~===Normal mode operation characterization===~~	+
-	In normal mode, AOM is controlled by our LabView program. Voltage input for RF signal is from –ve1 Volt to –ve5 Volts in –ve.1 Volt increment. 1st order diffracted beam power is recorded for every ascending voltage increment for .5W, 1.5W, 2W and 2.5W input laser powers. Different laser powers are used to check if any how the characteristic of the AOM is input power dependent, which it should not be. RF signal Vs diffracted beam power will help us in obtaining the best workable range of voltages over which power increases linearly. I will also help us in characterizing the relationship between the voltage and diffracted power. The data is presented below:	+
-	~~{{ShowGoogleExcel\|id=0ApjWjFYiQdkfdDhNLXZOMUZwYXpONzhIU3V3MElicHc\|width=800\|height=600}}~~	+
-		+
-	~~====Result:====~~	+
-	*Data Sheet 1 and Chart 1: By looking the chart it’s clear; diffracted beam power is not linearly related with voltage. It has strange characteristic, which is same for all laser powers: So there is no laser power dependence and any laser power can be chosen to define the AOM characteristic. Characteristic: It runs somewhat exponentially in the beginning from 1 to 1.4 volts, somewhat linear between 1.5 to 3.1 volts (the two straight vertical lines on the chart represents that) and second degree polynomial in the end from 3.2 to 5 volts. '''''So the most appropriate workable range for linear power modulation (in relatively same size of steps) is from 1.5 to 3.1 Volts at any input laser power.'''''	+
-		+
-	* Data Chart3: Shows how power increases in % over 1 to 5 Volts at 2W of laser power. By joining the head of each histogram the characteristic curve can be traced out. Between 1.5 and 3.1 Volt the power increases almost in same step size of avg 3.45% (.069W) /step in comparison to .8% (not linear; over range of 1 to 1.4 Volts) and .42% (not linear; over range of 3.1 to 5 Volt). '''''3.45% step size is more convenient for power modulation and power is also linear over the steps.'''''	+
-		+
-	* Data Chart 2: Shows power step in %; the difference between the two consecutive power-increments over the difference in the two consecutive voltage increments (.1 Volt; steps). It gives us the better idea of over what range of voltage, the steps are over all large with somewhat of same histogram height difference. The region between 1.5 to 3.21 Volts contains that.	+
-	[[Category:~~AOM~~]]	+

Pranav Rathi at 16:31, 15 November 2012

Pranav Rathi — Thu, 15 Nov 2012 16:31:11 GMT

←Older revision		Revision as of 16:31, 15 November 2012
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-	~~{\|{{table}} width="800"~~	+	[[/Characterization of AOM module]]
-	\|-	+
-	~~\|style="background-color: #EEE"\|~~[[~~Image:owwnotebook_icon.png\|128px]]<span style="font-size:22px;"> Project name<~~/~~span>~~	+
-	~~\|style="background-color: #F2F2F2" align="center"\|<html><img src="/images/9/94/Report.png" border="0" /></html> [[{{#sub:{{FULLPAGENAME}}\|0\|-11}}\|Main project page~~]]<br />{{#if:{{#lnpreventry:{{FULLPAGENAME}}}}\|<html><img src="/images/c/c3/Resultset_previous.png" border="0" /></html>[[{{#lnpreventry:{{FULLPAGENAME}}}}{{!}}Previous entry]]<html>      </html>}}{{#if:{{#lnnextentry:{{FULLPAGENAME}}}}\|[[{{#lnnextentry:{{FULLPAGENAME}}}}{{!}}Next entry]]<html><img src="/images/5/5c/Resultset_next.png" border="0" /></html>}}	+
-	\|-	+
-	~~\| colspan="2"\|~~	+
-	~~<!-- ##### DO NOT edit above this line unless you know what you are doing. ##### -->~~	+
	==AOM Characterization==		==AOM Characterization==
	===Introduction:===		===Introduction:===

Pranav Rathi: /* Result: */

Pranav Rathi — Thu, 15 Nov 2012 16:28:27 GMT

Result:

←Older revision		Revision as of 16:28, 15 November 2012
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	* Data Chart 2: Shows power step in %; the difference between the two consecutive power-increments over the difference in the two consecutive voltage increments (.1 Volt; steps). It gives us the better idea of over what range of voltage, the steps are over all large with somewhat of same histogram height difference. The region between 1.5 to 3.21 Volts contains that.		* Data Chart 2: Shows power step in %; the difference between the two consecutive power-increments over the difference in the two consecutive voltage increments (.1 Volt; steps). It gives us the better idea of over what range of voltage, the steps are over all large with somewhat of same histogram height difference. The region between 1.5 to 3.21 Volts contains that.
-	[[Category:~~Optical Tweezer~~]]	+	[[Category:AOM]]

Pranav Rathi: /* Result: */

Pranav Rathi — Sat, 15 May 2010 15:44:46 GMT

Result:

←Older revision		Revision as of 15:44, 15 May 2010
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	{{ShowGoogleExcel\|id=0ApjWjFYiQdkfdHZ1VTdkaGFGbDFnSmtpUHJGdzR5aWc\|width=800\|height=500}}		{{ShowGoogleExcel\|id=0ApjWjFYiQdkfdHZ1VTdkaGFGbDFnSmtpUHJGdzR5aWc\|width=800\|height=500}}
	====Result:====		====Result:====
-	The relationship is linear. So the AOM gives output power in 1st order diffracted beam, of average around 70% of the input power (in CW mode). This help us calculating the usable power of any input power without measuring; for example if I set the laser on .10W, then the usable power at the tweezer is 70% of it, which is .07W or 70mW.The maximum usable power for the tweezer is 2.66W. If we want to stay in the single mode operation regime, it is 1.4W (at room temperature). When the laser is cooled down to 60F, it is stretched to 1.9W (2.75W input).	+	'''''The relationship is linear. So the AOM gives output power in 1st order diffracted beam, of average around 70% of the input power (in CW mode).''''' This help us calculating the usable power of any input power without measuring; for example if I set the laser on .10W, then the usable power at the tweezer is 70% of it, which is .07W or 70mW.The maximum usable power for the tweezer is 2.66W. If we want to stay in the single mode operation regime, it is 1.4W (at room temperature). When the laser is cooled down to 60F, it is stretched to 1.9W (2.75W input).

	===Normal mode operation characterization===		===Normal mode operation characterization===

Pranav Rathi: /* Result: */

Pranav Rathi — Sat, 15 May 2010 15:40:53 GMT

Result:

←Older revision		Revision as of 15:40, 15 May 2010
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	*Data Sheet 1 and Chart 1: By looking the chart it’s clear; diffracted beam power is not linearly related with voltage. It has strange characteristic, which is same for all laser powers: So there is no laser power dependence and any laser power can be chosen to define the AOM characteristic. Characteristic: It runs somewhat exponentially in the beginning from 1 to 1.4 volts, somewhat linear between 1.5 to 3.1 volts (the two straight vertical lines on the chart represents that) and second degree polynomial in the end from 3.2 to 5 volts. '''''So the most appropriate workable range for linear power modulation (in relatively same size of steps) is from 1.5 to 3.1 Volts at any input laser power.'''''		*Data Sheet 1 and Chart 1: By looking the chart it’s clear; diffracted beam power is not linearly related with voltage. It has strange characteristic, which is same for all laser powers: So there is no laser power dependence and any laser power can be chosen to define the AOM characteristic. Characteristic: It runs somewhat exponentially in the beginning from 1 to 1.4 volts, somewhat linear between 1.5 to 3.1 volts (the two straight vertical lines on the chart represents that) and second degree polynomial in the end from 3.2 to 5 volts. '''''So the most appropriate workable range for linear power modulation (in relatively same size of steps) is from 1.5 to 3.1 Volts at any input laser power.'''''

-	* Data Chart3: Shows how power increases in % over 1 to 5 Volts at 2W of laser power. By joining the head of each histogram the characteristic curve can be traced out. Between 1.5 and 3.1 Volt the power increases almost in same step size of avg 3.45% (.069W) /step in comparison to .8% (not linear; over range of 1 to 1.4 Volts) and .42% (not linear; over range of 3.1 to 5 Volt). '''''3.45% step size is more convenient for power modulation and power is also linear over the ~~step size~~.'''''	+	* Data Chart3: Shows how power increases in % over 1 to 5 Volts at 2W of laser power. By joining the head of each histogram the characteristic curve can be traced out. Between 1.5 and 3.1 Volt the power increases almost in same step size of avg 3.45% (.069W) /step in comparison to .8% (not linear; over range of 1 to 1.4 Volts) and .42% (not linear; over range of 3.1 to 5 Volt). '''''3.45% step size is more convenient for power modulation and power is also linear over the steps.'''''

	* Data Chart 2: Shows power step in %; the difference between the two consecutive power-increments over the difference in the two consecutive voltage increments (.1 Volt; steps). It gives us the better idea of over what range of voltage, the steps are over all large with somewhat of same histogram height difference. The region between 1.5 to 3.21 Volts contains that.		* Data Chart 2: Shows power step in %; the difference between the two consecutive power-increments over the difference in the two consecutive voltage increments (.1 Volt; steps). It gives us the better idea of over what range of voltage, the steps are over all large with somewhat of same histogram height difference. The region between 1.5 to 3.21 Volts contains that.
	[[Category:Optical Tweezer]]		[[Category:Optical Tweezer]]

Pranav Rathi: /* Result: */

Pranav Rathi — Sat, 15 May 2010 04:36:41 GMT

Result:

←Older revision		Revision as of 04:36, 15 May 2010
Line 27:		Line 27:

	====Result:====		====Result:====
-	*Data Sheet 1 and Chart 1: By looking the chart it’s clear; diffracted beam power is not linearly related with voltage. It has strange characteristic, which is same for all laser powers: So there is no laser power dependence and any laser power can be chosen to define the AOM characteristic. Characteristic: It runs somewhat exponentially in the beginning from 1 to 1.4 volts, somewhat linear between 1.5 to 3.1 volts (the two straight vertical lines of the chart ~~reprsents~~ that) and second degree polynomial in the end from 3.2 to 5 volts. '''''So the most appropriate workable range for linear power modulation (in relatively same size of steps) is from 1.5 to 3.1 Volts at any input laser power.'''''	+	*Data Sheet 1 and Chart 1: By looking the chart it’s clear; diffracted beam power is not linearly related with voltage. It has strange characteristic, which is same for all laser powers: So there is no laser power dependence and any laser power can be chosen to define the AOM characteristic. Characteristic: It runs somewhat exponentially in the beginning from 1 to 1.4 volts, somewhat linear between 1.5 to 3.1 volts (the two straight vertical lines on the chart represents that) and second degree polynomial in the end from 3.2 to 5 volts. '''''So the most appropriate workable range for linear power modulation (in relatively same size of steps) is from 1.5 to 3.1 Volts at any input laser power.'''''

	* Data Chart3: Shows how power increases in % over 1 to 5 Volts at 2W of laser power. By joining the head of each histogram the characteristic curve can be traced out. Between 1.5 and 3.1 Volt the power increases almost in same step size of avg 3.45% (.069W) /step in comparison to .8% (not linear; over range of 1 to 1.4 Volts) and .42% (not linear; over range of 3.1 to 5 Volt). '''''3.45% step size is more convenient for power modulation and power is also linear over the step size.'''''		* Data Chart3: Shows how power increases in % over 1 to 5 Volts at 2W of laser power. By joining the head of each histogram the characteristic curve can be traced out. Between 1.5 and 3.1 Volt the power increases almost in same step size of avg 3.45% (.069W) /step in comparison to .8% (not linear; over range of 1 to 1.4 Volts) and .42% (not linear; over range of 3.1 to 5 Volt). '''''3.45% step size is more convenient for power modulation and power is also linear over the step size.'''''

Pranav Rathi: /* Result: */

Pranav Rathi — Sat, 15 May 2010 04:35:15 GMT

Result:

←Older revision		Revision as of 04:35, 15 May 2010
Line 27:		Line 27:

	====Result:====		====Result:====
-	*Data Sheet 1 and Chart 1: By looking the chart it’s clear; diffracted beam power is not linearly related with voltage. It has strange characteristic, which is same for all laser powers: So there is no laser power dependence and any laser power can be chosen to define the AOM characteristic. Characteristic: It runs somewhat exponentially in the beginning from 1 to 1.4 volts, somewhat linear between 1.5 to 3.1 volts and second degree polynomial in the end from 3.2 to 5 volts. '''''So the most appropriate workable range for linear power modulation (in relatively same size of steps) is from 1.5 to 3.1 Volts at any input laser power.'''''	+	*Data Sheet 1 and Chart 1: By looking the chart it’s clear; diffracted beam power is not linearly related with voltage. It has strange characteristic, which is same for all laser powers: So there is no laser power dependence and any laser power can be chosen to define the AOM characteristic. Characteristic: It runs somewhat exponentially in the beginning from 1 to 1.4 volts, somewhat linear between 1.5 to 3.1 volts (the two straight vertical lines of the chart reprsents that) and second degree polynomial in the end from 3.2 to 5 volts. '''''So the most appropriate workable range for linear power modulation (in relatively same size of steps) is from 1.5 to 3.1 Volts at any input laser power.'''''

	* Data Chart3: Shows how power increases in % over 1 to 5 Volts at 2W of laser power. By joining the head of each histogram the characteristic curve can be traced out. Between 1.5 and 3.1 Volt the power increases almost in same step size of avg 3.45% (.069W) /step in comparison to .8% (not linear; over range of 1 to 1.4 Volts) and .42% (not linear; over range of 3.1 to 5 Volt). '''''3.45% step size is more convenient for power modulation and power is also linear over the step size.'''''		* Data Chart3: Shows how power increases in % over 1 to 5 Volts at 2W of laser power. By joining the head of each histogram the characteristic curve can be traced out. Between 1.5 and 3.1 Volt the power increases almost in same step size of avg 3.45% (.069W) /step in comparison to .8% (not linear; over range of 1 to 1.4 Volts) and .42% (not linear; over range of 3.1 to 5 Volt). '''''3.45% step size is more convenient for power modulation and power is also linear over the step size.'''''

Pranav Rathi: /* Result: */

Pranav Rathi — Fri, 14 May 2010 22:34:30 GMT

Result:

←Older revision		Revision as of 22:34, 14 May 2010
Line 32:		Line 32:

	* Data Chart 2: Shows power step in %; the difference between the two consecutive power-increments over the difference in the two consecutive voltage increments (.1 Volt; steps). It gives us the better idea of over what range of voltage, the steps are over all large with somewhat of same histogram height difference. The region between 1.5 to 3.21 Volts contains that.		* Data Chart 2: Shows power step in %; the difference between the two consecutive power-increments over the difference in the two consecutive voltage increments (.1 Volt; steps). It gives us the better idea of over what range of voltage, the steps are over all large with somewhat of same histogram height difference. The region between 1.5 to 3.21 Volts contains that.
		+	[[Category:Optical Tweezer]]

Pranav Rathi: /* Result: */

Pranav Rathi — Fri, 14 May 2010 18:27:50 GMT

Result:

←Older revision		Revision as of 18:27, 14 May 2010
Line 27:		Line 27:

	====Result:====		====Result:====
		+	*Data Sheet 1 and Chart 1: By looking the chart it’s clear; diffracted beam power is not linearly related with voltage. It has strange characteristic, which is same for all laser powers: So there is no laser power dependence and any laser power can be chosen to define the AOM characteristic. Characteristic: It runs somewhat exponentially in the beginning from 1 to 1.4 volts, somewhat linear between 1.5 to 3.1 volts and second degree polynomial in the end from 3.2 to 5 volts. '''''So the most appropriate workable range for linear power modulation (in relatively same size of steps) is from 1.5 to 3.1 Volts at any input laser power.'''''
		+
		+	* Data Chart3: Shows how power increases in % over 1 to 5 Volts at 2W of laser power. By joining the head of each histogram the characteristic curve can be traced out. Between 1.5 and 3.1 Volt the power increases almost in same step size of avg 3.45% (.069W) /step in comparison to .8% (not linear; over range of 1 to 1.4 Volts) and .42% (not linear; over range of 3.1 to 5 Volt). '''''3.45% step size is more convenient for power modulation and power is also linear over the step size.'''''
		+
		+	* Data Chart 2: Shows power step in %; the difference between the two consecutive power-increments over the difference in the two consecutive voltage increments (.1 Volt; steps). It gives us the better idea of over what range of voltage, the steps are over all large with somewhat of same histogram height difference. The region between 1.5 to 3.21 Volts contains that.

Pranav Rathi: /* Normal mode operation characterization */

Pranav Rathi — Thu, 13 May 2010 19:35:44 GMT

Normal mode operation characterization

←Older revision		Revision as of 19:35, 13 May 2010
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	In normal mode, AOM is controlled by our LabView program. Voltage input for RF signal is from –ve1 Volt to –ve5 Volts in –ve.1 Volt increment. 1st order diffracted beam power is recorded for every ascending voltage increment for .5W, 1.5W, 2W and 2.5W input laser powers. Different laser powers are used to check if any how the characteristic of the AOM is input power dependent, which it should not be. RF signal Vs diffracted beam power will help us in obtaining the best workable range of voltages over which power increases linearly. I will also help us in characterizing the relationship between the voltage and diffracted power. The data is presented below:		In normal mode, AOM is controlled by our LabView program. Voltage input for RF signal is from –ve1 Volt to –ve5 Volts in –ve.1 Volt increment. 1st order diffracted beam power is recorded for every ascending voltage increment for .5W, 1.5W, 2W and 2.5W input laser powers. Different laser powers are used to check if any how the characteristic of the AOM is input power dependent, which it should not be. RF signal Vs diffracted beam power will help us in obtaining the best workable range of voltages over which power increases linearly. I will also help us in characterizing the relationship between the voltage and diffracted power. The data is presented below:
	{{ShowGoogleExcel\|id=0ApjWjFYiQdkfdDhNLXZOMUZwYXpONzhIU3V3MElicHc\|width=800\|height=600}}		{{ShowGoogleExcel\|id=0ApjWjFYiQdkfdDhNLXZOMUZwYXpONzhIU3V3MElicHc\|width=800\|height=600}}
		+
		+	====Result:====