Changes

# ''warping'' -- This is increasingly a problem as diamond thickness is reduced.  Whole-crystal rocking curve broadening on the order of several mrad (compare with GlueX requirement of 20 μrad RMS) were seen in all 3 crystals less than 20 microns thick that were examined at CHESS.  Two of these had never been exposed to an electron beam, so the warping cannot be attributed to radiation damage.  A technique must be found to thin diamonds down to 20 microns that does not result in a free-standing crystal that is this badly warped, or else a mounting technique must be found which can hold the crystal flat once it has been thinned to 20 microns.

# ''warping'' -- This is increasingly a problem as diamond thickness is reduced.  Whole-crystal rocking curve broadening on the order of several mrad (compare with GlueX requirement of 20 μrad RMS) were seen in all 3 crystals less than 20 microns thick that were examined at CHESS.  Two of these had never been exposed to an electron beam, so the warping cannot be attributed to radiation damage.  A technique must be found to thin diamonds down to 20 microns that does not result in a free-standing crystal that is this badly warped, or else a mounting technique must be found which can hold the crystal flat once it has been thinned to 20 microns.

As an intermediate step in the above investigations, we needed to find a way to hold diamond samples in the target holder at CHESS that could hold the diamonds in the beam without significant stress or risk of vibration.  An elegant solution to this problem was found in the form of a pair of tightly-stretched mylar films attached to aluminum rings.  The sample is placed in the middle of one of the mylar films, then the other film is placed over it like a sandwich and the two rings bolted together.  Van der Waals forces between the sample and the diamond are sufficient to prevent the sample from moving between the mylar sheets while the target is rotated in the goniometer.  The fabrication technique described below is capable of producing stretched films whose flatness in the central 1 cm region is better than 20 μrad RMS, and whose fundamental resonance is in the vicinity of 1 kHz.

 

As an intermediate step in the above investigations, we needed to find a way to hold diamond samples in the target holder at CHESS, and allow samples to be moved in and out of the mount without risk of breaking the samples or damaging the mount.  The first design was a stretched wire mount similar to the one used to hold diamonds in the Hall B target ladder at Jlab.

* [[Hardware for Mounting of Diamond Radiators]] - [[User:Senderovich|Igor Senderovich]]

:* [[Hardware for Mounting of Diamond Radiators]] - [[User:Senderovich|Igor Senderovich]]

* [[Mylar Stretching for Diamond Mounting]] - [[User: mcintyre|James McIntyre]]

However, this proved not to work, due to excessive vibrations.  An elegant solution to this problem was found in the form of a pair of tightly-stretched mylar films attached to aluminum rings.  The sample is placed in the middle of one of the mylar films, then the other film is placed over it like a sandwich and the two rings bolted together.  Van der Waals forces between the sample and the diamond are sufficient to prevent the sample from moving between the mylar sheets while the target is rotated in the goniometer.  The fabrication technique described below is capable of producing stretched films whose flatness in the central 1 cm region is better than 20 μrad RMS, and whose fundamental resonance is in the vicinity of 1 kHz.

:* [[Mylar Stretching for Diamond Mounting]] - [[User: mcintyre|James McIntyre]]