Multiple reference OCT system
View Patent ↗The invention provides for generating a set of signature signals that correspond to a range of depths within a target. These signature signals can include multiple individual reference signals and be can modified to compensate for specific characteristics of the target. In the preferred embodiment the members of the set of signature signals are correlated with data sets by phase rotating individual reference signals to determine maximum and minimum correlation and thereby enabling determination of the scattering characteristic of the target at each depth. Also a pilot signal is monitored to dynamically determine the phase relationship between individual reference signals and thereby avail of phase sensitive detection techniques to enhance SNR at deeper regions where multiple individual reference signals exist.
1. A multiple reference optical coherence tomography system comprising:
a radiation source, generating reference radiation and probe radiation;
a detector, which detects radiation;
an electronic controller, said controller providing timing signals, and an electronic processor which interacts with said controller by means of electronic signals;
a first beam splitter, said first beamsplitter in the path of said reference radiation;
an optical element, said optical element comprising:
a first partially reflecting surface, where said first partially reflecting surface reflects at least eighty percent of said reference radiation;
a second partially reflecting surface, where said second partially reflecting surface reflects less than ten percent of said reference radiation, and
where said first and said second partially reflecting surfaces are in the pathway of said reference radiation and are separated by a preselected thickness of fused silica;
a reference mirror, said reference mirror mounted on a translational device where said translational device moves co-linearly with said reference radiation, and
where said translational motion is modulated by a periodic electronic drive signal from said controller, and
wherein a pilot signal is derived from interference signals generated by interference between reference radiation reflected by said second partially reflecting surface, in combination with high order reflections between said mirror and said first partially reflecting surface, and
said electronic processor monitors said pilot signal to dynamically determine parameters of signature signals, said signature signals representing a set of interference signals resulting from reference radiation interacting with scattered probe radiation associated with a plurality of depth points in a target of interest, and
where said electronic processor rotates the phase of at least one of the components of said signature signals, computes a difference between a maximum and minimum correlation value to generate a set of final correlation values, and generates a depth scan of said target with improved signal to noise ratio.
2. The system of claim 1 , wherein
said first beam splitter is polarized and orientated with respect to the polarization vector of said radiation source to direct radiation to said target and to said reference mirror, and wherein
said system further includes a quarter wave plate, said quarter wave plate positioned between said first beamsplitter and said target so that probe radiation is directed through said quarter wave plate to said target, and where said quarter wave plate is rotated to maximize the scattered probe radiation that is scattered back through the quarter wave plate, and said quarter wave plate has a polarization vector that maximizes radiation transmission through said first beam splitter towards said detector,
and wherein
said reference mirror rotates the polarization vector of the multiple reference radiation so that at least some of the radiation reflected from said reference mirror is directed by said first beam splitter towards said detector and a preselected amount of radiation reflected by said second partial reflective surface, whose polarization vector is zero rotated, is transmitted straight through the beam splitter and away from said detector.
3. The system of claim 2 , further including:
a second detector;
a half wave plate in the optical path between said first beamsplitter and said first and second detector;
a second beamsplitter, said second beamsplitter polarized and in the optical path between the said half wave plate and said first and second detector;
a turning mirror between said second beamsplitter and said second detector, such that
co-propagating and orthogonally polarized scattered probe and reference radiation pass through said half wave plate to said second polarized beam splitter which directs one polarization component of said scattered probe and reference radiation to said first detector and transmits the other polarization component to said turning mirror which directs a second component of said scattered probe and reference radiation to said second detector, such that said first and said second detectors enable said electronic processor to perform balanced detection, reduce common mode noise, and enhance signal processing and correlation with said set of signature signals.
4. The system as in claim 3 , further including:
a third beamsplitter, said third beamsplitter in the optical path of said first beamsplitter and said radiation source;
a third detector, said third detector positioned in the optical path of said third beam splitter and connected to said electronic processor,
where a portion of said reference radiation passing through said first beam splitter is directed said third beam splitter towards said third detector and then to said electronic processor for extraction of said pilot signal.
5. A multiple reference optical coherence tomography system, where said system is electrically coupled to electronics performing control and processing functions, and said comprising:
a radiation source, generating reference radiation and probe radiation;
a first beam splitter, said first beamsplitter in the path of said reference radiation;
an optical element, said optical element comprising:
a first partially reflecting surface, where said first partially reflecting surface reflects at least eighty percent of said reference radiation;
a second partially reflecting surface, where said second partially reflecting surface reflects less than ten percent of said reference radiation, and
where said first and said second partially reflecting surfaces are in the pathway of said reference radiation and are separated by a preselected thickness of fused silica;
a reference mirror, said reference minor mounted on a translational device where said translational device moves co-linearly with said reference radiation, and
where said translational motion is modulated by a periodic electronic drive signal; and
a first detector,
wherein a pilot signal is derived from interference signals generated by interference between reference radiation reflected by said second partially reflecting surface, in combination with high order reflections between said mirror and said first partially reflecting surface, and
said processor monitors said pilot signal to dynamically determine parameters of signature signals, said signature signals representing a set of interference signals resulting from reference radiation interacting with scattered probe radiation associated with a plurality of depth points in a target of interest, and
where said processor rotates the phase of at least one of the components of said signature signals, computes a difference between a maximum and minimum correlation value to generate a set of final correlation values, and generates a depth scan of said target with improved signal to noise ratio.
6. The system of claim 5 , wherein
said first beam splitter is polarized and orientated with respect to the polarization vector of said radiation source to direct radiation to said target and to said reference mirror,
and said system further includes a quarter wave plate, said quarter wave plate positioned between said first beamsplitter and said target so that probe radiation is directed through said quarter wave plate to said target, and where said quarter wave plate is rotated to maximize the scattered probe radiation that is scattered back through the quarter wave plate, and said quarter wave plate has a polarization vector that maximizes radiation transmission through said first beam splitter towards said detector,
and wherein
said reference mirror rotates the polarization vector of the multiple reference radiation so that at least some of the radiation reflected from said reference mirror is directed by said first beam splitter towards said detector and a preselected amount of radiation reflected by said second partial reflective surface, whose polarization vector is zero rotated, is transmitted straight through the beam splitter and away from said detector.
7. The system of claim 6 , further including:
a second detector;
a half wave plate in the optical path between said first beamsplitter and said first and second detector;
a second beamsplitter, said second beamsplitter polarized and in the optical path between the said half wave plate and said first and second detector;
a turning mirror between said second beamsplitter and said second detector such that
co-propagating and orthogonally polarized scattered probe and reference radiation pass through said half wave plate to said second polarized beam splitter which directs one polarization component of said scattered probe and reference radiation to said first detector and transmits the other polarization component to said turning minor which directs a second component of said scattered probe and reference radiation to said second detector, such that said first and said second detectors enable said processor to perform balanced detection, reduce common mode noise, and enhance signal processing and correlation with said set of signature signals.
8. The system as in claim 7 , further including:
a third beamsplitter, said third beamsplitter in the optical path of said first beamsplitter and said radiation source; and
a third detector, said third detector positioned in the optical path of said third beam splitter and connected to electronic processor, so that
a portion of said reference radiation passing through said first beam splitter is directed said third beam splitter towards said third detector and then to said electronic processor for extraction of said pilot signal.