epr resonators 5 - chemical instrumentationcavities are characterized by their q or quality factor,...

User Service Training Course

EPR Resonators 5

Why Do We Use Resonators? 5.1In optical spectroscopy, spectra are usually acquired by simply shining lightthrough the sample and detecting how much light gets through. (SeeFigure 5-1.) This technique is unfortunately not very effective for EPR spec-troscopy. The reason is that an optical absorption spectrum is much strongerthan an EPR absorption spectrum. We need a little help to see our weak EPRsignals. Optical absorptions are stronger for two reasons:

1. Population differences between the two energy levels involved in thetransition are greater for optical spectroscopy, resulting in more intenseabsorptions. The greater population difference is a consequence of theBoltzmann population distribution of the energy levels.

2. Optical absorptions are usually electric dipole transitions and EPRspectra are usually magnetic dipole transitions. The magnetic dipoletransitions usually have a smaller transition moment (i.e. are weaker)than electric dipole transitions.

In order to enhance sensitivity, we use microwave resonators. These resona-tors are usually cavities. (Note: all cavities are resonators but not all resona-tors are cavities, for example, split ring and dielectric resonators.) A cavity isa metal box in which the microwaves can bounce around. A resonator helpsincrease sensitivity by “focusing” or “concentrating” the microwave power atthe sample and storing the microwave energy. The next section explains howthis happens as well as some of the basic ideas needed to troubleshoot EPRresonators.

Figure 5-1 A simple optical spectrometer.

Basic Concepts of EPR Resonators

5-2

Basic Concepts of EPR Resonators 5.2In this section, we shall discuss the properties of EPR cavities and howchanges in these properties due to absorption result in an EPR signal. Amicrowave cavity is simply a metal box with a rectangular or cylindricalshape which resonates with microwaves much as an organ pipe resonateswith sound waves. Resonance means that the cavity stores the microwaveenergy; therefore, at the resonance frequency of the cavity, no microwaveswill be reflected back, but will remain inside the cavity. (See Figure 5-2.)

Cavities are characterized by their Q or quality factor, which indicates howefficiently the cavity stores microwave energy. As Q increases, the sensitivityof the spectrometer increases. The Q factor is defined as:

, [5-1]

where the energy dissipated per cycle is the amount of energy lost during onemicrowave period. Energy can be lost to the side walls of the cavity becausethe microwaves generate electrical currents in the side walls of the cavitywhich in turn generates heat. We can measure Q factors easily because thereis another way of expressing Q:

, [5-2]

where νres is the resonant frequency of the cavity and ∆ν is the width at halfheight of the resonance.

A consequence of resonance is that there will be a standing wave inside thecavity. Standing electromagnetic waves have their electric and magnetic fieldcomponents exactly out of phase, i.e. where the magnetic field is maximum,the electric field is minimum and vice versa. The spatial distribution of theamplitudes of the electric and magnetic fields in a commonly used EPR cav-ity is shown in Figure 5-3. We can use the spatial separation of the electricand magnetic fields in a cavity to great advantage. Most samples havenon-resonant absorption of the microwaves via the electric field (this is how amicrowave oven works) and the Q will be degraded by an increase in the dis-sipated energy. It is the magnetic field that drives the absorption in EPR.Therefore, if we place our sample in the electric field minimum and the mag-

Figure 5-2 Reflected microwave power from a resonant cavity.

∆ν

νν

Q 2π(energy stored)energy dissipated per cycle-----------------------------------------------------------------=

Qνres∆ν--------=

Basic Concepts of EPR Resonators

User Service Training Course 5-3

netic field maximum, we obtain the biggest signals and the highest sensitiv-ity. The cavities are designed for optimal placement of the sample.

We couple the microwaves into the cavity via a hole called an iris. The size ofthe iris controls the amount of microwaves which will be reflected back fromthe cavity and how much will enter the cavity. The iris accomplishes this bycarefully matching or transforming the impedances (the resistance to thewaves) of the cavity and the waveguide (a rectangular pipe used to carrymicrowaves). There is an iris screw in front of the iris which allows us toadjust the “matching”. This adjustment can be visualized by noting that as thescrew moves up and down, it effectively changes the size of the iris. (SeeFigure 5-4.)

How do all of these properties of a cavity give rise to an EPR signal? Whenthe sample absorbs the microwave energy, the Q is lowered because of theincreased losses and the coupling changes because the absorbing samplechanges the impedance of the cavity. The cavity is therefore no longer criti-cally coupled and microwave will be reflected back to the bridge, resulting inan EPR signal.

Figure 5-3 Magnetic and electric field patterns in a standard EPR cavity.

Figure 5-4 The matching of a microwave cavity to a waveguide.

A More Technical Description

5-4

A More Technical Description 5.3A more detailed explanation now follows for those who are more technicallyminded. An equivalent circuit diagram for a reflection cavity is shown inFigure 5-5. L,C, and r form the equivalent circuit for the resonator. L and Cdetermine the resonant frequency and r (the losses in the walls and the sam-ple) determines the unloaded Q:

. [5-3]

The transformer (with n = turns ratio) represents the iris and iris screw; ittransforms the impedance of the microwave source, R0 to the impedance ofthe cavity r. Moving the iris screw (with the metal stub on the end) down-wards effectively increases the turn ratio in the equivalent circuit.

The iris lets microwaves enter the cavity but also lets microwaves leak out aswell. The power leaking out is proportional to R0n2. Combining the twolosses (losses in the cavity as well as leakage out of the cavity), a new Q,called the loaded Q, can be defined:

. [5-4]

It is useful to define yet another parameter, the coupling coefficient:

. [5-5]

The coupling coefficient conveniently defines three conditions. β = 1 corre-sponds to a critically coupled or “matched” cavity. This corresponds to maxi-mum power transfer from the microwave source to the cavity. MaximumEPR sensitivity is achieved in this condition. The VSWR (Voltage Standing

Figure 5-5 The equivalent circuit of a reflection cavity.

QuωL

r--------=

QLωL

R0n2 r+---------------------=

βR0n2

r------------=



Wave Ratio) is equal to 1, which corresponds to a reflection coefficient Γ, ofzero where

. [5-6]

This means when we are matched, no microwaves are reflected from the cav-ity. It also means (See Equation [5-4].) that the loaded Q is half the unloadedQ. β < 1 corresponds to an undercoupled cavity with VSWR = 1/β and Γ > 0.This means that microwaves are reflected from the cavity. Equation [5-4] alsotells us that the Q is somewhat higher than for a matched cavity. β > 1 corre-sponds to an overcoupled cavity with VSWR = β and Γ< 0. Microwaves arereflected from the cavity with a 180 degree phase shift. Equation [5-4] pre-dicts that the Q is lower than for a matched cavity.

Armed with the above equations, we can now investigate what happens whenwe observe an EPR spectrum. We start with a matched cavity. When the sam-ple absorbs microwaves, it effectively increases r, the equivalent resistance ofthe cavity. From Equation [5-5] and Equation [5-6], it is apparent that thecavity becomes undercoupled and reflects microwaves back to the bridge.The reflected microwaves are the EPR spectra observed with the spectrome-ter.

The preceding equations also help us understand what we are doing whilematching the cavity. We usually start with an undercoupled cavity. The modepicture on the spectrometer (with the reference arm turned off) looks similarto Figure 5-6.

The coupling coefficient is not 1, therefore some microwaves are reflectedback from the cavity. (See Equation [5-5] and Equation [5-6].) As we lowerthe iris screw, the dip will drop towards the baseline and eventually meet it(See Figure 5-7.), indicating critical coupling (i.e. no microwaves reflectedback.).

Figure 5-6 The mode picture of an undercoupled cavity.

Figure 5-7 The mode picture of a matched cavity.

Γ VSWR-1VSWR+1-----------------------=


5-6

Lowering the iris screw corresponds to increasing the turns ratio n in theequivalent circuit shown in Figure 5-5. If the iris screw is still further low-ered, the cavity becomes overcoupled. The Q therefore decreases and micro-waves are reflected back. (See Equation [5-4] through Equation [5-6] andFigure 5-8.) The lower Q can be seen from the width of the cavity resonance.

Sometimes, if the iris is even further lowered, we can once again match andundercouple the cavity. This is not particularly mysterious if you studyFigure 5-9.

The metal stub on the end of the iris screw is in equivalent positions for ahigh and low iris screw position. The disadvantage of the lower position isthat the microwaves have to pass through the lossy plastic of the iris screw.Figure 5-9 also suggests a solution if you are having problems matching yourcavity. If you use a larger iris tip, you can change the effective size of the irismore, resulting in a greater coupling range.

Larger iris tips are particularly useful for lossy samples. Lossy samples (usu-ally) interact with the electric field of the microwaves to heat the sample. Thiseffect is similar to heating food in a microwave oven. Examples of lossy sam-ples are polar liquids such as water, sulfuric acid, chloroform, and methanol.Sometimes, semiconductor samples exhibit such effects. This non-resonant

Figure 5-8 The mode picture of an overcoupled cavity.

Figure 5-9 Two equivalent positions of an iris screw.



absorption of microwaves increases r. The Q of the cavity therefore drops,thereby decreasing the sensitivity of the spectrometer. The increased value ofr also makes it more difficult to match the cavity. A larger n, the turns ratio inthe equivalent circuit, is required to match the cavity. The larger turn ratiocorresponds to moving the iris screw downwards.

In order to avoid placing our samples in the electric field of the cavity, weneed to know the field distributions inside the cavity. The distributionsdepend on the shape and the “mode” of the different cavities. These proper-ties determine the utility of a particular cavity for a specific sample.

The most commonly used cavity in EPR has been the rectangular TE102 cav-ity. The Bruker ER 4102ST is such a cavity. The squares of the microwavemagnetic and electric fields are displayed in Figure 5-10. The electric andmagnetic fields are constant across the cavity. Note that the maxima in thepeaks of the electric and magnetic fields are out of phase with each other. Wetherefore can place our sample simultaneously in a magnetic field maximumand an electric field minimum. The sample holders on the ER 4102ST aredesigned such that the sample and sample tube lies in the “valley” betweenthe two electric field “mountains”. Note that if you have a small sample,moving the sample up and down will change the microwave magnetic fieldseen by the sample. It is therefore important, particularly for small samples,to center the sample in the cavity at the magnetic field maximum. TheER 4102ST cavity is a good “universal” resonator. It is easy to use with cryo-genics. Large modulation amplitudes can be obtained.

The second most popular cavity has been the cylindrical TM110 cavity. Thecorresponding cavities in the Bruker product line are the ER 4103TM andER4108 TMH cavities. The squares of the microwave magnetic and electricfields are displayed in Figure 5-11. The electric and magnetic fields are con-stant across the cavity. The sample holders on both cavities are designed suchthat the sample and sample tube lies in the “valley” between the two electricfield “mountains”. The ER 4103TM cavity is used predominately for flat cellwork. A flat cell is a thin and flat sample tube for working with lossy liquidssuch as water. The advantage of this cavity over the ER 4102ST for such

Figure 5-10 The field distribution in a TE102 rectangular cavity.


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samples is that much more sample can be put in the peak magnetic field partsof the cavity and the Q is higher. The ER 4108TMH is a thinner version ofthe ER 4103TM with no irradiation grids and smaller openings for sampleinsertion. It has a higher Q than the ER 4103TM, making it more sensitive. Italso has a larger filling factor. The filling factor is an indication of the volumeof the sample in the magnetic field peaks compared to the volume of the cav-ity. The higher it is, the more sensitive the cavity becomes. The disadvantageof the ER 4108TMH is that the smaller openings make cryogenic work moreproblematic.

The other type of cavity offered by Bruker is the cylindrical TE011 cavity.There are many special cavities offered by Bruker which have this mode.Among them are the ER 4106 ZR, ER 4107WZ, and ER 4115OD resonators.The ER 4119HS and ER 4122SHQE cavities have a similar mode, but withsome proprietary modifications. These cavities have very high Q’s and henceare very sensitive cavities for low loss samples. Also, if you use proper aque-ous sample cells such as AquaX, very high sensitivity can be attained forlossy samples. This is why the ER 4119HS and ER 4122SHQE cavities arecurrently the standard resonators for the EMX and Elexsys spectrometersrespectively.

The squares of the microwave magnetic and electric fields of the TE011 modeare displayed in Figure 5-12. The sample holders on both cavities aredesigned such that the sample and sample tube lies in the “valley” betweenthe two electric field “mountains”. The dielectric resonator can be considereda special case of this type of cavity. It consists of some high dielectric con-stant material, which concentrates the microwave fields in a much smallervolume. This results in a much better filling factor.

Figure 5-11 The field distribution in a TM110 cylindrical cavity.



Figure 5-12 The field distribution in a TE011 cylindrical cavity.

a) Side profile of magnetic field.

b) Axial profile of magnetic field in center of cavity.

c) Side profile of electric field.

d) Axial profile of electric field in center of cavity.

Common Problems

5-10

Common Problems 5.4

No Cavity Dip 5.4.11. Waveguide gasket installed improperly. See Figure 5-13 for the

proper orientation of the gasket.

2. Cavity undercoupled or overcoupled. First, look at the micro-wave frequency where you normally expect the cavity to resonate andthen adjust the iris screw for better coupling. This can occur whenworking with lossy samples such as aqueous solutions in flat cells orcapillaries.

3. You need more microwave power. If you are using insufficientmicrowave power, it can be difficult to see the cavity dip. We recom-mend setting the microwave attenuator to at least 35 dB for the bestvisibility.

Unable to Critically Couple Cavity 5.4.21. Sample position. If too much of a lossy sample is in the microwave

electric field in the cavity, you will not be able to critically couple thecavity. Move the sample until the coupling becomes better. This is par-ticularly important for flat cells and capillaries.

2. Microwave reference phase. If the microwave reference phase isnot set properly, you will not be able to critically couple the cavity.Retune the microwave bridge properly.

3. Iris tip size. When working with lossy samples, it is advisable to usea larger iris tip to increase the coupling range of the cavity. This is par-ticularly important when working with flat cells or capillaries.

4. Condensation on the cryostat. Make sure that you purge the cav-ity with dry Nitrogen if you are operating with a cryostat at tempera-tures lower than room temperatures.

Figure 5-13 Correct and incorrect installation of waveguide gasket.

Common Problems


Baseline Distortion 5.4.31. Linear baseline drifts. The use of very large modulation fields can

produce large eddy currents in the cavity side walls. These currents caninteract with the magnetic field to produce a torque on the cavity andcreate a resonant frequency shift. A linear field dependent or modula-tion amplitude dependent baseline is indicative of such an effect. Thisphenomenon should not be observed if the cavity end plates are prop-erly fitted and torqued. Do not attempt to adjust the torque on theplates. Contact your local Bruker EPR service representative.

2. Slowly and randomly varying baseline. The use of high micro-wave power or large modulation fields can heat the cavity and the sam-ple. The ensuing thermal drifts in the coupling of the cavity, as well asthe frequency of the cavity, can result in a fluctuating offset in the sig-nal. Allow the tuned cavity and sample to come to thermal equilibriumbefore performing the final tuning of the cavity. Once the cavity isequilibrated and properly tuned under the equilibrated condition, youcan start acquiring a spectrum. Avoid air drafts around the cavity, asthey can randomly change the temperature of the cavity and sampleand hence the baseline of the spectrum.

3. Variable temperature operation. Cavity frequency and couplinginstability may be induced during variable temperature operation, espe-cially at very low or very high temperatures. Increase the flow rate ofthe cavity and waveguide purging gas as the operating temperaturedeparts further from room temperature. Wait for the cavity to stabilizeat each new operating temperature before recording the spectrum.Retune the cavity to compensate for any frequency shift and re-estab-lish critical coupling at each temperature.

4. Background signal. Your cavity, cryostat, sample tube, or samplemay be contaminated. (See Section 5.5 to learn how to clean cavities.)

Excessive Noise Output 5.4.41. Microphonic generated noise. Secure the waveguide and cavity

assembly by using the plastic waveguide stabilizers. Secure the samplefirmly in the collet. If you use a cryostat, make sure that the cryostatsits firmly in the cavity. Make sure that an excessive flow rate throughthe cryostat does not vibrate the sample.

2. Worn iris screw. Check for a worn iris coupling screw. An iris screwthat does not fit snugly in the waveguide may generate noise by modu-lating the cavity coupling. Replace the worn iris screw with a new one.

3. Boiling liquids. If you are using a dewar with a boiling refrigerantsuch as liquid nitrogen, you must increase the AFC modulation level.

Common Problems

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Poor Sensitivity 5.4.51. Wrong cavity type for sample. The type of cavity you use for a

particular sample can make a large difference in sensitivity. Consultthe Bruker literature on the full line of EPR cavities to determine whichone is best for your samples.

2. Low cavity Q. The cavity Q can be degraded because of impropersample positioning. Sample in the microwave electric field will reducethe sensitivity by degrading the cavity Q, especially for high dielectricloss samples. This can happen if you are using flat cells or capillaries.

3. Cavity not critically coupled. Maximum power is transferredbetween the cavity and waveguide when the cavity properly matchesthe impedance of the waveguide, i.e., is critically coupled. A drasti-cally undercoupled iris will not transmit power to the cavity and so willnot excite EPR transitions. A drastically overcoupled cavity will have alower Q, resulting in lower sensitivity. These effects can happen whenusing lossy samples such as aqueous solutions or conducting samples.

4. Water condensation. During low temperature operation, water cancondense inside the cavity. Water, being a high dielectric loss material,will destroy the cavity Q and absorb the microwave power in the cav-ity. Avoid condensation by using a purging nitrogen gas flow throughthe cavity.

5. Sample not properly positioned. Make sure that your sample isproperly positioned in the cavity. The sample should be at the center ofthe cavity.

Lineshape Distortion 5.4.61. High conductivity. High conductivity exhibited by samples with

mobile electrons will result in asymmetric lines known as Dysonianlineshapes. This results from a mixing of the absorption and dispersionsignals in these samples.

2. Lossy samples. If you put large lossy samples in a cavity, you canalso obtain Dysonian lineshapes. Use progressively smaller capillariesuntil you obtain a symmetric lineshape.

3. Background signal. A strong background signal from contamina-tion of the EPR cavity or the sample can produce distortions.

No Signal When Everything Works 5.4.71. Check cables. Make sure that all the cables are connected. Check

the modulation cable and the preamplifier cable.

2. Sample position. If you have a small sample, make sure that thesample is centered in the cavity.

3. Magnetic field values. Are you using the correct field values to seeyour EPR signal? If you are using a cryostat, remember that the micro-wave frequency drops and hence the field for resonance will also belower.

Cavity Cleaning


Cavity Cleaning 5.5Sometimes a sample may break in the cavity and contaminate the cavity. Theadage “An ounce of prevention is worth a pound of cure.” is very appropriatehere. Take care when inserting and removing samples tubes. Make sure youclean the outside of your sample tubes before insertion. Use a nitrogen cry-ostat; that way, the easily cleaned cryostat is contaminated instead of the cav-ity. Contaminants may also come from the lab as well. Maintain thecleanliness of your lab. Avoid smoking near the cavity. Keep the cavitysealed up with the solid collet plugs and the irradiation grid cover plate whenit is not in use.

To test if your cavity background complies with the specifications, consultChapter 13 to learn how to run a background test.

Cavities can be cleaned in some cases. Care must be taken because some ofthe solvents can damage paint on the waveguide or damage the cavity itself. Itis easiest to clean the cavity if you know what the contaminant is and in whatit is soluble. This knowledge is easily available if you are the one who actu-ally contaminated the cavity. Alas, your colleagues usually will not admit tobreaking any sample tubes in the cavity. Therefore there are instructions forwashing away many different types of contaminants. If the cleaning proce-dures do not succeed, contact your local Bruker EPR service representativefor advice.

ER 4102ST Style Resonators 5.5.1ER 4102ST, ER 4103TM, ER 4108TMH, ER 4116DM, and ER 4105DR canbe cleaned with the following procedure.

1. Blow the cavity out. Remove the collet nuts and collets as well asany irradiation grid cover. Use a stream of clean high pressure nitrogento dislodge or blow out any contamination. Direct the gas stream downthe collet stacks and through the irradiation grid (if present). Do notuse compressed air because it can often be contaminated with oil,water and other substances. Run another background test as describedin Chapter 13. If the background is not within specification after thetreatment, proceed to the next step.

2. Wash the cavity out with toluene. Place a solid collet piece on thebottom of the cavity and tighten the collet nut. Put the irradiation gridcover plate on the front of the cavity. Fill the cavity with clean toluene.(Be careful as the toluene can strip the paint off the waveguide.) Shakethe cavity for a few minutes, taking care not to spill the solvent. Emptythe cavity of the solvent. This should wash away the most nonpolarcontaminants. The theory is to use a series of solvents of increasingpolarity. One of the solvents has a good chance of dissolving the dirt.

3. Wash the cavity out with acetone. Repeat the above procedurewith clean acetone. (Be careful as the acetone can strip the paint off thewaveguide.)

Cleaning ins t ruc-tions are specific fora cavity type. If yourcavity is not listed inthe cleaning instruc-tions, do not use thecleaning techniquesdescribed. You maydamage your cavity.When in doubt, con-t ac t you r l oca lBruker EPR servicerepresentative.

Wear safety glasseswhen cleaning yourcavity. Always washthe cavity with suffi-cient ventilation i.e.a hood. Wear glovesand avoid contactwith the solventsbecause t hey a r etoxic and irritating.Dispose of the sol-vents properly aftercleaning the cavity..

Cavity Cleaning

5-14

4. Wash the cavity out with methanol. Repeat the above procedurewith clean methanol. (Be careful as the methanol can strip the paint offthe waveguide.)

5. Wash the cavity out with distilled or deionized water. Repeatthe above procedure with distilled or deionized water.

6. Dry the cavity. Dry the cavity with a stream of dry clean Nitrogen orlet it dry overnight in a clean dry place.

7. Cleaning metal contamination. If you are certain that the contam-inant is a metal ion, a quick rinse with 0.1 M disodium EDTA followedby a thorough rinse of distilled or deionized water sometimes removesthe contaminant. Dry the cavity as described above.

ER 4119HS Style Resonators 5.5.2The ER 4119HS and ER 4122SHQE resonators are cleaned in a similar man-ner. It does differ in one respect; the cavity must not be filled. Remove boththe upper and lower collets. Turn the cavity upside down. Flow the solventsthrough the bottom collet stack using a pipette or wash bottle. Then dry thecavity with a stream of dry clean Nitrogen or let it dry overnight in a cleandry place.

Changing EPR Cavities


Changing EPR Cavities 5.6

Getting Ready (Elexsys) 5.6.1We assume that the spectrometer is turned on, connected, and an experimentloaded before performing the following operations.

1. Click the Activate button. If this button is not already activated,click its button in the Acquisition Control Tool section. (SeeFigure 5-14.) This button allows you to interactively control the spec-trometer when it is activated.

2. Click the Parameter button. Click this button to open the Acquisi-tion Parameter dialog box. (See Figure 5-14.)

3. Set the modulation amplitude to zero. Click the Signal Chan-nel tab. Enter a value of 0.00 in the Modulation Amplitude box. (SeeFigure 5-15.)

4. Set the magnetic field to the minimal value. Click the Absc.1:Field tab. Enter in a value of 0.00 in the Sweep Width box and thena value of 0.00 in the Center Field box.

Figure 5-14 The Activate and Parameter buttons.

Figure 5-15 Set the Modulation Amplitude to zero.

If the Open ParameterPanel button is grey,you can not open theParameter dialog box.Create or load an exper-iment so you can openthe Parameter dialogbox.

ParameterButton

ActivateButton

Setting the magneticfield to the minimumvalue avoids the risk ofmagnetizing your watchwhen changing cavities.


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5. Close the Acquisition Parameter dialog box. Click the Closebutton of the Acquisition Parameter dialog box. Click the Activatebutton again to exit the interactive control mode.

6. Open the Microwave Bridge Tuning dialog box. If this windowis not already open, click its button in the monitoring panel. The buttontoggles the dialog box open and closed. The Microwave Bridge Tun-ing dialog box will then appear. (See Figure 5-16.)

7. Switch the microwave bridge to Stand By mode. (SeeFigure 5-16.) Click the Stand By button in the dialog box to change tothe Stand By mode.

Figure 5-16 The Microwave Bridge Tuning dialog box.

Stand ByButton

MicrowaveBridge

TuningDialog

Box

Up IrisButton

Down IrisButton

Stand ByButton

AttenuationDisplay

ButtonTuning



Getting Ready (EMX) 5.6.21. Open the Interactive Spectrometer Control dialog box. If this

window is not already open, click its button (See Figure 5-17.) in thetool bar. The button toggles the dialog box open and closed. The Inter-active Spectrometer Control dialog box will then appear. (SeeFigure 5-18.)

2. Set the modulation amplitude to zero. Enter a value of 0.00 inthe Modulation Amplitude box.

3. Set the magnetic field to the minimal value. Enter in a value of0.00 in the Sweep Width box and a value of 0.00 in the Center Fieldbox.

4. Close the Interactive Spectrometer Control dialog box. Clickthe Interactive Spectrometer Control (the button labeled I) in thetool bar. The button toggles the dialog box on and off. The InteractiveSpectrometer Control dialog box will then disappear. (SeeFigure 5-17 and Figure 5-18.)

5. Open the Microwave Bridge Control dialog box. If this win-dow is not already open, click its button (See Figure 5-17.) in the toolbar. The button toggles the dialog box open and closed. The Micro-wave Bridge Control dialog box will then appear. (See Figure 5-19.)

Figure 5-17 The Interactive Spectrometer Control button.

InteractiveSpectrometer

ControlButton

MicrowaveBridgeControlButton

Figure 5-18 The Interactive Spectrometer Control dialog box.

Setting the magneticfield to the minimumvalue avoids the risk ofmagnetizing your watchwhen changing cavities.


5-18

6. Switch the microwave bridge to Stand By mode. Click theStand By button in the dialog box to change to the Stand By mode.(See Figure 5-19.)

Changing Cavities 5.6.31. Disconnect any accessories. If a variable temperature dewar

assembly is installed, disconnect the coolant transfer line and the ther-mocouple connections from the cavity.

2. Disconnect the modulation cable from the cavity. This is thetwin-ax cable labeled with a white connector and attached to the frontof the standard cavity. To remove it, push the connector in, turncounter-clockwise and gently pull the cable away. (See Figure 5-20.)

3. Disconnect the rapid scan cable from the cavity. Disconnectthe 50 Gauss rapid scan cable if it is connected to the cavity. This is thetwin-ax cable labeled with a yellow connector and attached to the frontleft of the standard cavity.

4. Disconnect the nitrogen purge line from the port on thewaveguide. The port is half way down the waveguide attached to thecavity. (See Figure 5-20.)

Figure 5-19 The Microwave Bridge Control dialog box.

AttenuationDisplay

IrisButtons

Stand ByButton

Not all cavities have arapid scan cable.



5. Disconnect the iris motor shaft from the iris screw. Firstunscrew the lock nut from the iris screw. Lift the shaft upwards to dis-connect. Move the iris motor to the side where it is out of the way. (SeeFigure 5-21.)

Figure 5-20 Connections on the ER 4122SHQ cavity.

Figure 5-21 Disconnecting the iris motor shaft from the iris screw.

IrisScrew

ModulationCable

IrisMotor

IrisMotorShaft

NitrogenPurgePort

WaveguideGasket

WaveguideScrews

Store the lock nut in aplace where it will notbe lost.

IrisMotorShaft

LockNut


5-20

6. Disconnect the cavity. While grasping the waveguide attached tothe cavity with one hand, unscrew the four waveguide screws joiningthe two sections of waveguide. (See Figure 5-20.) Loosen thewaveguide stabilizers by rotating the screws and carefully remove thecavity from the air gap of the magnet. (See Figure 5-22.) Take care notto lose the gasket which was between the two wave guide flanges.Remove the waveguide stabilizers. (See Figure 5-23.) Seal the cavitywith the solid collets and put the cavity in a safe clean place.

7. Install the waveguide stabilizers on the new cavity. (SeeFigure 5-23.) Visually position them just above the magnet pole caps.

8. Attach the appropriate size collet and pedestal on the cav-ity.

9. Screw in the iris. Manually (By hand!) turn the iris screw almost allthe way in. The iris screw will stop rotating. Back the screw out at leastone turn after it hits the bottom. This will further decrease yourchances of accidentally breaking the iris screw during the tune proce-dure.

10. Connect the modulation cable to the cavity. (See Figure 5-20.)

11. Connect the 50 Gauss Rapid Scan cable to the cavity. (Elex-sys only.) If you plan to do rapid scan experiments and there arerapid scan coils on your cavity, connect the 50 G rapid scan cable (theyellow twinax cable) to the front left connector of the cavity.

Figure 5-22 Loosening the waveguide stabilizers.

Figure 5-23 Removing/Installing the waveguide stabilizers.Steps 9. and 15. areused to set the l imitswi tches in the i r i sm ot o r. The l i m i tswitches prevent youfrom screwing the iris intoo fa r and therebybreaking the iris screw.

Make sure you connectthe modulation cable tothe MOD (modulation)connector and not theR.S. (Rapid Scan) con-nector. Not all cavitieshave rapid scan coils.



12. Reconnect the waveguide sections and tighten the stabiliz-ers. Do not forget to install the waveguide flange gasket between thetwo flanges; make sure it is oriented correctly. (See Figure 5-24.) Posi-tion the cavity in the center of the magnet air gap by moving the bridgeon the table. Carefully tighten the stabilizers. Be careful not to stressthe waveguide when expanding the stabilizers. Reconnect the nitrogenpurge line and adjust the flow rate for a light flow.

13. Reposition the iris motor. Move the iris motor into a position suchthat the iris motor shaft hangs freely in the magnet. It should not be incontact with other objects.

Finishing Up (Elexsys) 5.6.41. Lower the iris motor. Open the Microwave Bridge Tuning dialog

box. Click the Options button.

Figure 5-24 Installing the waveguide gasket properly.

Figure 5-25 Iris controls in the Microwave Bridge Tuning dialog box.

Options

Iris UpButton

Iris DownButton


5-22

A dialog box for lowering the iris screw appears. (See Figure 5-26.)

Click the button next to Iris Run Down. A message reminding you todisconnect the iris motor pops up. Heed the message and then click theYes button to close the dialog box. (See Figure 5-27.) The iris motorwill turn until it reaches the lower limit. Click Close on the Iris Con-trol dialog box when the iris motor stops. You can also manually lowerthe iris motor. Click and hold the Iris Down button. In the MicrowaveBridge Tuning dialog box (See Figure 5-25.), activate the Iris Downbutton until the iris motor stops; this is the lower limit of the motor.

2. Reconnect the iris motor shaft to the iris screw. The proce-dure here is like Step 5. performed in reverse. Reposition the irisscrew motor. Screw the lock nut on the iris screw. Click and hold theup iris button in the Microwave Bridge Tuning dialog box (SeeFigure 5-16.) until the iris screw is approximately 0.5 to 1 cm. abovethe top surface of the cavity body.

Figure 5-26 The Iris Control dialog box.

Figure 5-27 Make sure disconnecting the iris motor.

T he end o f t h e i r i smotor shaft should fiteasily in the top of theiris screw. If it does not,rotate the ir is screwuntil it fits easily.



3. Read in the calibration file for the cavity. Click Acquisition inthe menu bar and then click Spectrometer Configuration. (SeeFigure 5-28.) The Spectrometer Configuration dialog box will thenappear. (See Figure 5-29.)

Click the Signal Channel tab. In the Standard Calibration folderthere is a box called Calibration Data Set. Click the arrow to view thedrop-down list. Select the appropriate calibration file for your cavityand click the Apply button at the bottom of the folder. This will auto-matically load the calibration data you have selected.

Figure 5-28 The Spectrometer Configuration button.

SpectrometerConfiguration

Button

Figure 5-29 Selecting a calibration file.

ChangeFile


5-24

Confirm that the calibration file is the correct one for the cavity. Thecalibration file name usually consists of two or three letters that iden-tify the type of cavity (ST for ER 4102ST or TM for ER 4103TM) fol-lowed by the serial number of the cavity. This number is found on theback or front of the cavity. Click Close to exit. If you can not find thecalibration file for the cavity you need to do the calibration first. Fol-low the instruction in Chapter 2 of the Elexsys E 500 User’s Manual:Advanced Operations to create a calibration file.

Finishing Up (EMX) 5.6.51. Click and hold the down Iris Button. Activate this button (See

Figure 5-19.) until the iris motor stops turning; this is the lower limitof the motor.

2. Reconnect the iris motor shaft to the iris screw. The proce-dure here is like Step 5. performed in reverse. Reposition the irisscrew motor. Screw the lock nut on the iris screw. Click and hold theup iris button in the Microwave Bridge Tuning dialog box (SeeFigure 5-19.) until the iris screw is approximately 0.5 to 1 cm. abovethe top surface of the cavity body.

3. Read in the calibration file for the cavity. Open the ExperimentOptions dialog box in order to read in the calibration information. Ifthis window is not already open, click its button (See Figure 5-30.) inthe tool bar. The button toggles the dialog box open and closed. TheExperiment Options dialog box will then appear. Click on theChange File button. A new dialog box, Open Calibration File willappear. Select the appropriate calibration file for your cavity and clickOK. This will automatically load the calibration data you haveselected. Confirm that the calibration file is the correct one for the cav-ity. The calibration file name usually consists of two or three lettersthat identify the type of cavity (ST for ER 4102ST or TM forER 4103TM) followed by the serial number of the cavity. This numberis located on either the front or back of the cavity. Clicking Cancelreturns you to the Experiment Options dialog box.

T he end o f t h e i r i smotor shaft should fiteasily in the top of theiris screw. If it does not,rotate the ir is screwuntil it fits easily.

B1 Conversion


Serv ice eng ineers o f ten save the ca l ib ra t ion f i l e s in thec:\...\acquisit\tpu directory during the installation of the spectrometer.

B1 Conversion 5.7The resonator converts microwave power into B1 (microwave magnetic mag-netic field) at the sample. Each type of resonator has a different conversionefficiency. The following table helps you to calculate an approximate B1value for different types of resonators.

The values are calculated by using the following equation:

, [5-7]

where C is the constant in the table and P is the microwave power. To takeinto account different bandwidths the C’ constant can be used in the follow-ing equation:

, [5-8]

where ∆ν is the bandwidth of the resonator.

Figure 5-30 The Experiment Options and Open Calibration Filedialog boxes.

ChangeFile

B1[G] C P[W]⋅=

B1[G] C' P[W]⋅∆ν[MHz]

----------------------------=

B1 Conversion

5-26

B1 Conversion Mode Q C [G / √W] C’[G√MHz / √W]

ER 4102STStandard Rectangular

TE102 2500150

1.40.3 (overcoupled)

2.72.4

ER 4105DRDouble Rectangular

TE104 3000 0.6 1.1

ER 4104OROptical Transmission

TE103 3000 1.0 1.8

ER 4116DMDual Mode Resonator

TE102 ⊥ 3000 1.3 2.3

ER 4103TMCylindrical TM-Mode

TM110 3500 1.0 1.7

ER 4108TMHH i g h S e n s i t i v i t yTM-Mode

TM110 2500 1.2 2.4

ER 4106ZRCCylindrical Concentric

TE011 7500 1.5 1.7

ER 4115ODCOptical CylindricalConcentric

TE011 5000 1.3 1.8

ER 4122 SHQSuper High Q Resonator

N/A 7500 2.0 2.3

EN 801ENDOR Resonator

TM110 1000 0.7 2.2

ER 4118 X-MD5Dielectric Resonator

TE011 4000150


6.59

ER 4118 X-MS5Split Ring Resonator

N/A 500150


8.89.6

EN 4118 X-MD5Pulsed ENDOR Resonator

TE011 500150


7.98

Table 5-1 Conversion factors for Bruker EPR resonators.

epr resonators 5 - chemical instrumentationcavities are characterized by their q or quality factor,...

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