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Lab Assignment: Quantized Conductance Lab | ||||||||
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5. Statistical data analysis, build histogram, perform Gaussian fits to the histogram. 6. Develop understanding of quantum mechanics | ||||||||
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Part A: Data CollectionObserve quantum steps in the current vs distance (I-d) curve. You should be able to see at least one conductance (conductance=current/voltage) step at G0=2e^2/h≈77.5 microsiemen (uS) or R0=1/G0=12.9 kΩ, There are typically more than 1 steps, appearing at 1G0, 2G0, ... | ||||||||
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Write Up You need to explain the experiment principle and theory, quantum conductance, quantum tunneling. | ||||||||
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Lab Assignment: Quantized Conductance Lab | ||||||||
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< < | In this lab, you will explore the phenomena of quantized conductance in a gold nanocontact repeated created at room temperature. From the experiment, you will understand the importance of quantum mechanics at the nanoscale. You will also learn the typical electrical characterization techniques in condensed matter Physics and nano science fields. | |||||||
> > | Quantum mechanics states that electrons behave like waves. Howver, in macroscopic systems, we rarely observe their wavelike properties. For example, the electron transport in bulk metal can be well-expalined by the classical Drude's model. As the system becomes smaller and the temperature goes down, Drude’s model no longer explains the electronic transport. the wave properties of electroan appear. In this lab, you will explore the phenomena of quantized conductance in a gold quantum point contact repeatedly created at room temperature. From the experiment, you will understand the importance of quantum mechanics at the nanoscale. You will also learn the typical electrical characterization techniques in condensed matter Physics and nano science fields. | |||||||
TheoryPlease read the references(see the three attachments at the bottom of this page) to understand the quantized conductance through classical Physics (Drude model) and Quantum Physics. | ||||||||
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< < | Quantum conductance can also refer to Wikipedia: https://en.wikipedia.org/wiki/Conductance_quantum | |||||||
> > | Quantum conductance, denoted by the symbol G0, is the quantized unit of electrical conductance. It is defined by the elementary charge e and Planck constant h as G0=2e^2/h=7.7480917310(18)×10−5 S≈1/13 kΩ More information can refer to Wikipedia: https://en.wikipedia.org/wiki/Conductance_quantum You should also read refs about quantum tunneling. Quantum tunneling happens when the two metal electrodes are in a distance of a few nanometers. You will observe the quantum tunneling current right after the breakage of the gold point contact. Based on quantum tunnleing, Scanning Tunneling Microscope (STM) was invented and STM can help us to see individual atoms at real space. | |||||||
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< < | You can also read refs about quantum tunneling. | |||||||
Setup and calibrationBefore the experiment, you need to understand the theory and principle of the experiment. | ||||||||
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6. Develop understanding of quantum mechanics
Part A: Data Collection | ||||||||
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< < | Observe quantum steps in the current vs distance (I-d) curve. You should be able to see at least one conductance (conductance=current/voltage) step at G0=2e^2/h=77.5 microsiemen (uS) or R0=1/G0=12.9 kohm, There are typically more than 1 steps, appearing at 1G0, 2G0, 3G0... | |||||||
> > | Observe quantum steps in the current vs distance (I-d) curve. You should be able to see at least one conductance (conductance=current/voltage) step at G0=2e^2/h≈77.5 microsiemen (uS) or R0=1/G0=12.9 kΩ, There are typically more than 1 steps, appearing at 1G0, 2G0, ... | |||||||
Learn how to optimize the experimental conditions, i.e., tip approach and withdraw speed of the tip, applied bias, environment (in air and in solution). | ||||||||
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< < | Build histograms from 50, 100 and 200 I-d curves at 0.1V bias. Compare the shape of peaks. | |||||||
> > | Build histograms from 50, 100 and 200 I-d curves at 0.1V bias. Compare the shape of peaks and understand how the statistics play the role. | |||||||
Collect about 200 withdraw conductance curves (more is better) at different biases, 0.05V, 0.1V, 0.2V.
Part B: Data Analysis | ||||||||
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< < | You need to explain the experiment principle and theory. | |||||||
> > | You need to explain the experiment principle and theory, quantum conductance, quantum tunneling. | |||||||
The experimental setup: Simple diagram of electrical circuit of electrical measurement. How the gold point contact was repeatedly formed, the Piezoelectric effect. The precise control of distance by Piezo actuator. |
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Lab Assignment: Quantized Conductance Lab | ||||||||
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Please read the references(see the three attachments at the bottom of this page) to understand the quantized conductance through classical Physics (Drude model) and Quantum Physics. Quantum conductance can also refer to Wikipedia: https://en.wikipedia.org/wiki/Conductance_quantum | ||||||||
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> > | You can also read refs about quantum tunneling. | |||||||
Setup and calibrationBefore the experiment, you need to understand the theory and principle of the experiment. | ||||||||
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You will learn: | ||||||||
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< < | 1. How to prepare sharp gold tip and clean both gold tip and gold substrate | |||||||
> > | 1. How to prepare sharp(a few nanometer at the tip) gold tip and clean both gold tip and gold substrate | |||||||
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< < | 2. How the experimental setup works. | |||||||
> > | 2. How the experimental setup works (electric circuit, noise reduction...). | |||||||
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< < | 3. How to repeatedly acquire the conductance-distance data. | |||||||
> > | 3. Data acquisition using DAQ card (from national instrument) and customed labview programs | |||||||
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< < | 3. Data acquisition using NI DAQ and labview programs | |||||||
> > | 4. How to repeatedly acquire a large number of the conductance-distance (I-d) curves. | |||||||
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< < | 4. Statistical data analysis, build histogram, perform Gaussian fits to the histogram. | |||||||
> > | 5. Statistical data analysis, build histogram, perform Gaussian fits to the histogram. | |||||||
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< < | 5. Develop understanding of quantum mechanics | |||||||
> > | 6. Develop understanding of quantum mechanics | |||||||
Part A: Data CollectionObserve quantum steps in the current vs distance (I-d) curve. You should be able to see at least one conductance (conductance=current/voltage) step at G0=2e^2/h=77.5 microsiemen (uS) or R0=1/G0=12.9 kohm, There are typically more than 1 steps, appearing at 1G0, 2G0, 3G0... | ||||||||
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Collect about 200 withdraw conductance curves (more is better) at different biases, 0.05V, 0.1V, 0.2V.
Part B: Data Analysis | ||||||||
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< < | You will use the labview programs to build histograms from your hundreds of conductance curves (conductance vs. distance). You need to understand how to covert individual conductance curves to conductance histograms. After buding conductance histograms, you will perform Gaussian fits to the conductance peaks in the histograms. You will discuss the goodness of fit using reduced chi-square. | |||||||
> > | You will use the labview programs to build conductance histograms from hundreds of I-d curves you collected. You need to understand how to covert the current unit Amper to quantume conductance unit G0 and how to convert individual I-d curves to G-d curves, then to a conductance histogram (pay attention to the bin size). After buding conductance histograms, you will perform Gaussian fits to the conductance peaks in the histograms. You will discuss the goodness of fit using reduced chi-square. | |||||||
Materials and Equipment:The list of necessary equipment is: | ||||||||
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< < | Write Up | |||||||
> > | Write Up | |||||||
You need to explain the experiment principle and theory. | ||||||||
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Other interesting discovers in your experiments.
Comments | ||||||||
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> > | ||||||||
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Lab Assignment: Quantized Conductance LabIn this lab, you will explore the phenomena of quantized conductance in a gold nanocontact repeated created at room temperature. From the experiment, you will understand the importance of quantum mechanics at the nanoscale. You will also learn the typical electrical characterization techniques in condensed matter Physics and nano science fields.Theory | ||||||||
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< < | Please read the references(see the three attachments at the bottom of this page) to understand the quantized conductance through classical Physics and Quantum Physics. | |||||||
> > | Please read the references(see the three attachments at the bottom of this page) to understand the quantized conductance through classical Physics (Drude model) and Quantum Physics. | |||||||
Quantum conductance can also refer to Wikipedia: https://en.wikipedia.org/wiki/Conductance_quantum
Setup and calibration | ||||||||
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3. Data acquisition using NI DAQ and labview programs 4. Statistical data analysis, build histogram, perform Gaussian fits to the histogram. | ||||||||
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> > | 5. Develop understanding of quantum mechanics | |||||||
Part A: Data CollectionObserve quantum steps in the current vs distance (I-d) curve. You should be able to see at least one conductance (conductance=current/voltage) step at G0=2e^2/h=77.5 microsiemen (uS) or R0=1/G0=12.9 kohm, There are typically more than 1 steps, appearing at 1G0, 2G0, 3G0... Learn how to optimize the experimental conditions, i.e., tip approach and withdraw speed of the tip, applied bias, environment (in air and in solution). | ||||||||
Changed: | ||||||||
< < | Build histograms from 10, 50 and 100 I-d curves at 0.1V bias. Compare the shape of peaks. | |||||||
> > | Build histograms from 50, 100 and 200 I-d curves at 0.1V bias. Compare the shape of peaks. | |||||||
Collect about 200 withdraw conductance curves (more is better) at different biases, 0.05V, 0.1V, 0.2V.
Part B: Data Analysis | ||||||||
Changed: | ||||||||
< < | You will use the labview programs to build histograms from your hundreds of conductance curves, perform Gaussian fits. You will discuss the goodness of fit. | |||||||
> > | You will use the labview programs to build histograms from your hundreds of conductance curves (conductance vs. distance). You need to understand how to covert individual conductance curves to conductance histograms. After buding conductance histograms, you will perform Gaussian fits to the conductance peaks in the histograms. You will discuss the goodness of fit using reduced chi-square. | |||||||
Materials and Equipment:The list of necessary equipment is:
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The cleanness of the tip and substrate is important to achieve better results. The size of gold atom? Why the electron transport through the gold wire with the width of one or a few gold atoms be limited? | ||||||||
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< < | Explain why the current decrease with the withdraw of the tip, the quantum steps, and the tunneling current between two nanoscale electrodes after the point contact is broken. | |||||||
> > | For individual conductance curve (or G-d cruve), explain why the current decrease with the withdraw of the tip. Explain the quantum steps, the sharp drop of the conductance after the step, also the quantum tunneling current between two nanoscale electrodes after the point contact is broken. | |||||||
Other interesting discovers in your experiments.
Comments |
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Lab Assignment: Quantized Conductance Lab | ||||||||
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< < | In this lab, you will explore the phenomena of quantized conductance in a gold nanocontact repeated created at room temperature. From the experiment, you will understand the importance of quantum mechanics at the nanoscale. | |||||||
> > | In this lab, you will explore the phenomena of quantized conductance in a gold nanocontact repeated created at room temperature. From the experiment, you will understand the importance of quantum mechanics at the nanoscale. You will also learn the typical electrical characterization techniques in condensed matter Physics and nano science fields. | |||||||
Theory | ||||||||
Changed: | ||||||||
< < | Please read the references(see the three attachments at the bottom of this page) to understand the quantized conductance through classical Physics and Quantum Physics | |||||||
> > | Please read the references(see the three attachments at the bottom of this page) to understand the quantized conductance through classical Physics and Quantum Physics. Quantum conductance can also refer to Wikipedia: https://en.wikipedia.org/wiki/Conductance_quantum | |||||||
Setup and calibrationBefore the experiment, you need to understand the theory and principle of the experiment. | ||||||||
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2. How the experimental setup works. | ||||||||
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< < | 3. How to acquire the conductance data. | |||||||
> > | 3. How to repeatedly acquire the conductance-distance data. | |||||||
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< < | 3. Data acquisition using NI DAQ and labview program | |||||||
> > | 3. Data acquisition using NI DAQ and labview programs | |||||||
4. Statistical data analysis, build histogram, perform Gaussian fits to the histogram.
Part A: Data Collection | ||||||||
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< < | observe quantum steps | |||||||
> > | Observe quantum steps in the current vs distance (I-d) curve. You should be able to see at least one conductance (conductance=current/voltage) step at G0=2e^2/h=77.5 microsiemen (uS) or R0=1/G0=12.9 kohm, There are typically more than 1 steps, appearing at 1G0, 2G0, 3G0... Learn how to optimize the experimental conditions, i.e., tip approach and withdraw speed of the tip, applied bias, environment (in air and in solution). | |||||||
Changed: | ||||||||
< < | Learn how to optimize the experimental conditions, i.e., tip approach and withdraw speed, applied bias. | |||||||
> > | Build histograms from 10, 50 and 100 I-d curves at 0.1V bias. Compare the shape of peaks. | |||||||
Collect about 200 withdraw conductance curves (more is better) at different biases, 0.05V, 0.1V, 0.2V.
Part B: Data Analysis | ||||||||
Changed: | ||||||||
< < | Histogram your conductance curves, Gaussian fits, discuss the results and the goodness of fit. | |||||||
> > | You will use the labview programs to build histograms from your hundreds of conductance curves, perform Gaussian fits. You will discuss the goodness of fit. | |||||||
Materials and Equipment:The list of necessary equipment is:
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< < |
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> > |
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< < | You need to explain the experiment principle, theory, the experimental setup (how the gold point contact was repeatedly formed), results and discussions. | |||||||
> > | You need to explain the experiment principle and theory. The experimental setup: How the gold point contact was repeatedly formed, the Piezoelectric effect. The precise control of distance by Piezo actuator. Results and discussions: The cleanness of the tip and substrate is important to achieve better results. Explain why the current decrease with the withdraw of the tip, the quantum steps, and the tunneling current between two nanoscale electrodes after the point contact is broken. Other interesting discovers in your experiments. | |||||||
Comments |
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Lab Assignment: Quantized Conductance LabIn this lab, you will explore the phenomena of quantized conductance in a gold nanocontact repeated created at room temperature. From the experiment, you will understand the importance of quantum mechanics at the nanoscale.Theory | ||||||||
Changed: | ||||||||
< < | Please read the following references to understand the quantized conductance through classical Physics and Quantum Physics ref 1. ref 2. ref 3. | |||||||
> > | Please read the references(see the three attachments at the bottom of this page) to understand the quantized conductance through classical Physics and Quantum Physics | |||||||
Setup and calibrationBefore the experiment, you need to understand the theory and principle of the experiment. | ||||||||
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< < | Title | |||||||
> > | Lab Assignment: Quantized Conductance Lab | |||||||
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< < | Article text.---+ Lab Assignment: Cosmic Ray Lab | |||||||
> > | In this lab, you will explore the phenomena of quantized conductance in a gold nanocontact repeated created at room temperature. From the experiment, you will understand the importance of quantum mechanics at the nanoscale.
Theory | |||||||
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< < | In this lab you will measure the cosmic ray flux as a function of the zenith angle and determine its shape by fitting your data with a function that represent theoretical expectations. Does it conform to those expectations?
Setup and calibration | |||||||
> > | Please read the following references to understand the quantized conductance through classical Physics and Quantum Physics | |||||||
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< < | Before you begin your flux measurements you should become familiar with the experimental apparatus. To do this we'll first perform a calibration of the Cosmic Telescope, basically determine what high voltage to use for the PMT input and then take measurements of count rates before we plunge into our flux measurements. | |||||||
> > | ref 1. | |||||||
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< < | First: Connect the HV supply to the PMTs and use the oscilloscope to find the output signal from the PMT. You will likely need to adjust the time scale or sweep (horizontal axis) and the voltage scale (vertical axis) on the scope. We expect output signals from the PMT to be 10-20 ns long and the output voltage to be a few millivolts for the Cosmic Ray telescope setup. You'll also need to set up the scope to self trigger on the output pulse; set the trigger to trigger on the channel the PMT output is on. Note that the output will only trigger the scope if it exceeds a set discriminator (disc) threshold (the "level" knob located on the trigger portion of the scope). Adjust the level knob to some fraction of the PMT's average output voltage. Since our PMT output voltage is negative you'll want to set the threshold below 0 V to display any events. | |||||||
> > | ref 2. | |||||||
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< < | Once you have your scope displaying multiple PMT pulses and have ascertained a reasonable value for your discriminator threshold you can take the PMT output and redirect it to the discriminator NIM module. As with the disc threshold on the scope the disc threshold on the NIM Module is used to filter out noise pulses from signal pulses. You can adjust the disc threshold on the NIM module by turning the tiny set screw hidden inside the whole labeled "THR". The threshold voltage can be read with a multimeter with leads connected to ground and the disc reading pad. | |||||||
> > | ref 3.
Setup and calibration | |||||||
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< < | Before you proceed with the experiments, PART A and B below lets first determine the proper input voltage to run the PMTs at, given the chosen disc threshold settings that you've selected. We do this to insure that the PMT pulses and thus count rates are stable across a sizable range of input voltages which may drift over the course of the experiment. We'll do this by measuring the count rate as a function of input voltage and look the input voltage that corresponds to start of the count plateau. | |||||||
> > | Before the experiment, you need to understand the theory and principle of the experiment. | |||||||
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< < | Begin by setting up the cosmic telescope by connecting the PMT output to the NIM discriminator then connect the disc output to the counter. Set the counter time window to collect a few 100 events. Make sure that you are counting real signals by insuring that the disc is set sufficiently high, check with the scope. Take count reading at various PMT input voltage and plot the results. Please DO NOT go beyond 2000 VOLTS. What you should see is that the count rates varies a lot when the voltage is set too high or too low. You'll want to use the a random event source, like the Sr 90 to insure you have real triggers instead of noise with proper disc setting. DO this for BOTH PMTs and provide in your lab report the plots you create.
Part A: Observation of Poisson and Gaussian distributions in radioactive decay of Sr 90. | |||||||
> > | You will be supervised by a graduate student to use the experimental setup and collect data. Please follow the instruction of the graduate student. | |||||||
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< < | You will only need to use one of the scintillator/PMTs for this part of the experiment. Decide on how to best setup your cosmic telescope viz. discr setting and HV input from the calibration setup above. | |||||||
> > | You will learn: | |||||||
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< < | Using a random source, that 90 Sr is as good a random source as any. Take 100 measurements with the count time interval set to collect on average 1 event per time interval. Histogram the results. Your histogram will have on the horizontal axis the number of counts per interval and on the vertical axis the number of times you record a particular number of counts. How is the data distributed? Then repeat the exercise but now use 100 events per time interval. You can adjust any of the experimental conditions you control to achieve these measurements. You can change the distance between the source and the scintillator or adjust the discriminator level. What ever you do make sure you retain the randomness of the events by insuring you are not picking up PMT or other sources of noise. There is no need to fit the distributions in this part of the lab but please do feel free to comment on what you observe.
Part B: Cosmic Ray Flux | |||||||
> > | 1. How to prepare sharp gold tip and clean both gold tip and gold substrate | |||||||
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< < | Using both PMTs, both of which you should have already plateaued and are running in optimal configuration for your experiment, perform the flux vs. angle measurement. Here you'll need to use the coincide NIM module inline between the discriminator outputs and the counter. The coincidence counter will trigger and output a NIM pulse when it detects two NIM pulses. This particular coincidence counter uses the size of the input pulse to select the size of the window it will use to determine if there is a coincidence, check the manual for the device if you are interested in details, something you'll have to find online. As you take data do plot the distribution. In the SLAC paper, linked below you'll see an estimate of the count rate. Make sure your count rate is consistent with your expectation. It typically takes 20 minutes to take one reading and you don't want take 10 of these 20 min reading to find out you did something wrong. and fit a function form to your data and discuss what you see. There is a nice write up on this part that you can access as a reference. See document from SLAC linked below.
Equipment: | |||||||
> > | 2. How the experimental setup works. | |||||||
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< < | Our Cosmic Ray Telescope consists of a piece of plastic (organic) scintillator made out of material that when exposed to charged particles reacts by emitting light. The light travels through the transparent plastic material, reflecting from surfaces until eventually some of the photons emerge at the front face of the PMT. The PMT is an electronic device based on the photoelectric effect that first converts a small number photons, into an amplified electrical signal sufficiently large to be easily recorded by standard laboratory equipment. You should provide in your write up an a short description, longer than this, of how this works. You should also include a paragraph or two about cosmic rays, what are they where do they come from and what does our detector actually "see". | |||||||
> > | 3. How to acquire the conductance data. | |||||||
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< < | The list of necessary equipment is:
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> > | 3. Data acquisition using NI DAQ and labview program | |||||||
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< < | Include in your introduction a breif description of the important components of the apparatus you used to conduct this experiment:
Analysis | |||||||
> > | 4. Statistical data analysis, build histogram, perform Gaussian fits to the histogram.
Part A: Data Collection | |||||||
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< < | Histogram your flux measurments, number of counts vs. angle w.r.t zenith and fit the distribution with an appropriate probability distribution funciton. Discuss the results and the goodness of fit. | |||||||
> > | observe quantum steps | |||||||
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< < | GradingRubric
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> > | Learn how to optimize the experimental conditions, i.e., tip approach and withdraw speed, applied bias. | |||||||
Added: | ||||||||
> > | Collect about 200 withdraw conductance curves (more is better) at different biases, 0.05V, 0.1V, 0.2V.
Part B: Data Analysis | |||||||
Changed: | ||||||||
< < | -- Jorge Rodriguez - 2018-01-08 | |||||||
> > | Histogram your conductance curves, Gaussian fits, discuss the results and the goodness of fit.
Materials and Equipment:The list of necessary equipment is:
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Added: | ||||||||
> > | You need to explain the experiment principle, theory, the experimental setup (how the gold point contact was repeatedly formed), results and discussions. | |||||||
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> > |
TitleArticle text.---+ Lab Assignment: Cosmic Ray Lab In this lab you will measure the cosmic ray flux as a function of the zenith angle and determine its shape by fitting your data with a function that represent theoretical expectations. Does it conform to those expectations?Setup and calibrationBefore you begin your flux measurements you should become familiar with the experimental apparatus. To do this we'll first perform a calibration of the Cosmic Telescope, basically determine what high voltage to use for the PMT input and then take measurements of count rates before we plunge into our flux measurements. First: Connect the HV supply to the PMTs and use the oscilloscope to find the output signal from the PMT. You will likely need to adjust the time scale or sweep (horizontal axis) and the voltage scale (vertical axis) on the scope. We expect output signals from the PMT to be 10-20 ns long and the output voltage to be a few millivolts for the Cosmic Ray telescope setup. You'll also need to set up the scope to self trigger on the output pulse; set the trigger to trigger on the channel the PMT output is on. Note that the output will only trigger the scope if it exceeds a set discriminator (disc) threshold (the "level" knob located on the trigger portion of the scope). Adjust the level knob to some fraction of the PMT's average output voltage. Since our PMT output voltage is negative you'll want to set the threshold below 0 V to display any events. Once you have your scope displaying multiple PMT pulses and have ascertained a reasonable value for your discriminator threshold you can take the PMT output and redirect it to the discriminator NIM module. As with the disc threshold on the scope the disc threshold on the NIM Module is used to filter out noise pulses from signal pulses. You can adjust the disc threshold on the NIM module by turning the tiny set screw hidden inside the whole labeled "THR". The threshold voltage can be read with a multimeter with leads connected to ground and the disc reading pad. Before you proceed with the experiments, PART A and B below lets first determine the proper input voltage to run the PMTs at, given the chosen disc threshold settings that you've selected. We do this to insure that the PMT pulses and thus count rates are stable across a sizable range of input voltages which may drift over the course of the experiment. We'll do this by measuring the count rate as a function of input voltage and look the input voltage that corresponds to start of the count plateau. Begin by setting up the cosmic telescope by connecting the PMT output to the NIM discriminator then connect the disc output to the counter. Set the counter time window to collect a few 100 events. Make sure that you are counting real signals by insuring that the disc is set sufficiently high, check with the scope. Take count reading at various PMT input voltage and plot the results. Please DO NOT go beyond 2000 VOLTS. What you should see is that the count rates varies a lot when the voltage is set too high or too low. You'll want to use the a random event source, like the Sr 90 to insure you have real triggers instead of noise with proper disc setting. DO this for BOTH PMTs and provide in your lab report the plots you create.Part A: Observation of Poisson and Gaussian distributions in radioactive decay of Sr 90.You will only need to use one of the scintillator/PMTs for this part of the experiment. Decide on how to best setup your cosmic telescope viz. discr setting and HV input from the calibration setup above. Using a random source, that 90 Sr is as good a random source as any. Take 100 measurements with the count time interval set to collect on average 1 event per time interval. Histogram the results. Your histogram will have on the horizontal axis the number of counts per interval and on the vertical axis the number of times you record a particular number of counts. How is the data distributed? Then repeat the exercise but now use 100 events per time interval. You can adjust any of the experimental conditions you control to achieve these measurements. You can change the distance between the source and the scintillator or adjust the discriminator level. What ever you do make sure you retain the randomness of the events by insuring you are not picking up PMT or other sources of noise. There is no need to fit the distributions in this part of the lab but please do feel free to comment on what you observe.Part B: Cosmic Ray FluxUsing both PMTs, both of which you should have already plateaued and are running in optimal configuration for your experiment, perform the flux vs. angle measurement. Here you'll need to use the coincide NIM module inline between the discriminator outputs and the counter. The coincidence counter will trigger and output a NIM pulse when it detects two NIM pulses. This particular coincidence counter uses the size of the input pulse to select the size of the window it will use to determine if there is a coincidence, check the manual for the device if you are interested in details, something you'll have to find online. As you take data do plot the distribution. In the SLAC paper, linked below you'll see an estimate of the count rate. Make sure your count rate is consistent with your expectation. It typically takes 20 minutes to take one reading and you don't want take 10 of these 20 min reading to find out you did something wrong. and fit a function form to your data and discuss what you see. There is a nice write up on this part that you can access as a reference. See document from SLAC linked below.Equipment:Our Cosmic Ray Telescope consists of a piece of plastic (organic) scintillator made out of material that when exposed to charged particles reacts by emitting light. The light travels through the transparent plastic material, reflecting from surfaces until eventually some of the photons emerge at the front face of the PMT. The PMT is an electronic device based on the photoelectric effect that first converts a small number photons, into an amplified electrical signal sufficiently large to be easily recorded by standard laboratory equipment. You should provide in your write up an a short description, longer than this, of how this works. You should also include a paragraph or two about cosmic rays, what are they where do they come from and what does our detector actually "see". The list of necessary equipment is:
AnalysisHistogram your flux measurments, number of counts vs. angle w.r.t zenith and fit the distribution with an appropriate probability distribution funciton. Discuss the results and the goodness of fit. GradingRubric
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