BNMR: Helicity: Difference between revisions
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* [[BNMR]] | * [[BNMR]] | ||
* [[BNMR | * [[BNMR Dual Channel Mode|Dual Channel Mode]] | ||
* [[BNMR: Experimental Modes|Experimental Modes]] | * [[BNMR: Experimental Modes|Experimental Modes]] | ||
* [[BNMR: Getting Started|Getting Started]] | * [[BNMR: Getting Started|Getting Started]] | ||
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== Introduction == | == Introduction == | ||
The {{bnmqr|join=and}} experiments control the helicity via the PPG "POL DRV" output. The helicity is changed using a | The {{bnmqr|join=and}} experiments control the helicity via the PPG "POL DRV" output. The helicity is changed using a waveplate (Figure 1) that is moved into and out of the beam. The two helicity states are called "UP" and "DOWN". An experimental parameter ''flip helicity'' is provided for each [[BNMR#Experimental (PPG) Modes|Experimental Mode]]. When this is set to true, the helicity will be flipped. Some modes flip the helicity after each PPG cycle, others at the end of the scan. See [[BNMR Mode Parameters]] for details. | ||
[[Image:waveplate.png|400px|center|]] | |||
<br clear=all> | |||
<center> | |||
'''Figure 1''' Helicity Waveplate | |||
</center> | |||
== Helicity Switch Box == | == Helicity Switch Box == | ||
Since both experiments {{bnmqr|join=and}} control the same hardware (the helicity plate) signals from both experiments are connected to a helicity switch box (Rolf's box). | Since both experiments {{bnmqr|join=and}} control the same hardware (the helicity plate), signals to drive the helicity from both experiments are connected to a helicity switch box (Rolf's box), Figure 2. These signals are from each experiment's PPG "POL DRV" output. The electronics is edge-driven, so it only changes when it sees an edge. To ensure a particular helicity state at the begin-of-run in single channel mode (e.g. DOWN), the PPG must drive the helicity DOWN-UP-DOWN. In dual channel mode, it is not possible to ensure the required helicity in the way at the begin of run. It is assumed that by the second PPG cycle, the helicity will be in the correct state and the latched helicity readback provides confirmation. The first cycle is always discarded. | ||
These signals are from | |||
The experiment requests the helicity state for its next cycle by setting the PPG "POL DRV" output. In single channel mode, the helicity state is changed immediately. In dual channel mode, the helicity is not changed until that experiment receives the beam (see [[BNMR | The experiment requests the helicity state for its next cycle by setting the PPG "POL DRV" output. In single channel mode, the helicity state is changed immediately. In dual channel mode, the helicity is not changed until that experiment receives the beam (see [[BNMR Dual Channel Mode#Helicity]]). A circuit diagram of the helicity switch box as used for single and dual channel modes is shown in Figure 2b. (Figure 2a shows the original, single channel mode only). The D-type flip flops are edge driven, so they only change when an edge from the beam kicker signal is received. | ||
[[Image:helicity_switch_box.png|center|frame|Figure 2 Helicity Switch box]] | |||
<br clear=all> | |||
== Helicity Read Back == | == Helicity Read Back == | ||
Helicity read back signals have been provided in recent years so that the state of the helicity can be read with certainty, particularly in dual channel mode. The helicity state is read using a VMEIO32 | Helicity read back signals have been provided in recent years (Figure 1) so that the state of the helicity can be read with certainty, particularly in dual channel mode. The helicity state is read using a VME NIMIO32 register specially modified for the {{bnmqr|join=and}} experiments (see [[BNMR: DAQ Hardware Connections#NIMIO32|NIMIO32]] for details). Each experiment in provided with a VMEIO32 register. | ||
It provides a helicity readout for the present state of the helicity (used in single channel mode) as well as a latched helicity readout for dual channel mode. The latched readout latches the helicity state at the time that channel (BNMR or BNQR) has the beam. | |||
== Helicity test program == | |||
There is a helicity test program on both experiments {{Filepath|path=~/vmetest/heltest}} . This can be useful to diagnose problems when the helicity readback is not working. Usually it is found that a NIM bin is switched off, or a NIM module has failed. | |||
A simulator mode was also made to test the VME NIMIO32 modifications before the readback signals were available. This mode is not now used. | |||
[[Category:BNMR]] | [[Category:BNMR]] | ||
Revision as of 16:38, 8 June 2016
Links
Introduction
The bnmr and bnqr experiments control the helicity via the PPG "POL DRV" output. The helicity is changed using a waveplate (Figure 1) that is moved into and out of the beam. The two helicity states are called "UP" and "DOWN". An experimental parameter flip helicity is provided for each Experimental Mode. When this is set to true, the helicity will be flipped. Some modes flip the helicity after each PPG cycle, others at the end of the scan. See BNMR Mode Parameters for details.
Figure 1 Helicity Waveplate
Helicity Switch Box
Since both experiments bnmr and bnqr control the same hardware (the helicity plate), signals to drive the helicity from both experiments are connected to a helicity switch box (Rolf's box), Figure 2. These signals are from each experiment's PPG "POL DRV" output. The electronics is edge-driven, so it only changes when it sees an edge. To ensure a particular helicity state at the begin-of-run in single channel mode (e.g. DOWN), the PPG must drive the helicity DOWN-UP-DOWN. In dual channel mode, it is not possible to ensure the required helicity in the way at the begin of run. It is assumed that by the second PPG cycle, the helicity will be in the correct state and the latched helicity readback provides confirmation. The first cycle is always discarded.
The experiment requests the helicity state for its next cycle by setting the PPG "POL DRV" output. In single channel mode, the helicity state is changed immediately. In dual channel mode, the helicity is not changed until that experiment receives the beam (see BNMR Dual Channel Mode#Helicity). A circuit diagram of the helicity switch box as used for single and dual channel modes is shown in Figure 2b. (Figure 2a shows the original, single channel mode only). The D-type flip flops are edge driven, so they only change when an edge from the beam kicker signal is received.
Helicity Read Back
Helicity read back signals have been provided in recent years (Figure 1) so that the state of the helicity can be read with certainty, particularly in dual channel mode. The helicity state is read using a VME NIMIO32 register specially modified for the bnmr and bnqr experiments (see NIMIO32 for details). Each experiment in provided with a VMEIO32 register. It provides a helicity readout for the present state of the helicity (used in single channel mode) as well as a latched helicity readout for dual channel mode. The latched readout latches the helicity state at the time that channel (BNMR or BNQR) has the beam.
Helicity test program
There is a helicity test program on both experiments ~/vmetest/heltest . This can be useful to diagnose problems when the helicity readback is not working. Usually it is found that a NIM bin is switched off, or a NIM module has failed.
A simulator mode was also made to test the VME NIMIO32 modifications before the readback signals were available. This mode is not now used.