Abstract:
An apparatus for both deflecting a beam of light illuminating a spot on a surface and varying the size of the spot, electronically, without changing any system components. The apparatus includes an acousto-optic deflector (10) driven with a linear FM signal produced by a chirp signal generator (16). The linear FM signal is characterized with a dispersion rate, and the chirp signal generator includes a chirp dispersion selector to vary the dispension rate. A beam of collimated light (13) passes through the acousto-optic deflector (10) and appropriate focusing optics (14, 15) image the beam onto a spot in a nominal focal plane (17). The chirp dispension selector (17) sets the dispension rate in accord to a nominal rate, resulting in the beam illuminating a spot (18) in the focal plane (17). Generally, the focal plane coincides with a wafer surface (24), of the type having periodic (27b) and non-periodic (27c) features on it.
Abstract:
A surface height detection and positioning device for use in a surface inspection system. A light beam (25) impinges obliquely upon the surface (22), and a position detector (38) with a mechanical window (45) defining an aperture (46) receives specularly reflected light (33) producing a plurality of electrical signals. The aperture's width (46), along a scan direction, is of sufficient size to create a train of signals from each of the plurality of signals, having a frequency equal to the scan frequency. These signals carry information responsive to the position of the reflected beam (33) impinging on the detector and the beam's intensity. To abrogate information responsive to intensity variations at the detector, an electronic circuit (100) determines the sum and the difference of the plurality of signals, producing a summed signal and a difference signal, respectively. The difference signal is divided by the summed signal, thereby producing a normalized signal which represents the height of the surface.
Abstract:
A high throughput surface inspection system with enhanced detection sensitivity is described. The acquired data is processed in real time at a high rate of below 50 MHZ thereby reducing the cost for data processing. Anomalies are detected and verified by comparing adjacent repeating patterns and the height of the surface (40) is monitored and corrected dynamically to reduce misregistration errors between adjacent repeating patterns. Local thresholds employing neighborhood information are used for detecting and verifying the presence of anomalies. The sampled point spread function of the combined illumination (22) and collection system (90, 92, 111b) is exploited for anomaly detection and verification.
Abstract:
A broadband area-division beamsplitter that includes a pair of abutting triangular prisms (51 and 53) providing two surfaces that are in optical contact in certain areas and are out of optical contact in other areas. One prism surface (57) is substantially planar while adjoining surface (55) of the other prism has alternating protrusions and depressions. The two surfaces are oriented on a diagonal so that light incident through one of the other prism faces is incident on the adjoining surfaces at an angle larger than the critical angle, providing total internal reflection at the out-of-contact gap regions. The protrusions and depressions on the one prism surface may be in the form of a corrugation (Fig. 4) or a checkerboard (Fig. 5) or some other patterns.
Abstract:
An apparatus used to inspect patterned wafers (10) and other substrates with periodic features for the presence of particles, defects and other aperiodic features in which a spatial filter (26) placed in the Fourier plane is used in combination with either broadband illumination, angularly diverse illumination or both. Embodiments are described that illuminate a patterned substrate using (1) a single monochromatic source (210) with a slit-shaped aperture stop (207) for angularly diverse illumination, (2) a single broadband source (512) with a pinhole aperture stop (510) for broadband illumination, (3) a single broadband source (14) with a slit-shaped aperture stop (20) for both broadband and angularly diverse illumination, or (4) multiple sources (205, 210) with an aperture stop (20, 207) for each source for at least angularly diverse illumination. The spatial filters are characterized by opaque tracks (56; 656) in an otherwise transmissive filter for blocking the elongated bands produced by diffraction from the periodic features on the illuminated substrate.
Abstract:
A particle imager and method for imaging particles on surfaces of substrates (19). A reflective suface (17) is scanned by a collimated light beam (57) and particles on the surface are detected by the scattered light caused by the particles. During a scan path (81) the intensity of the scattered light is measured forming intensity traces (91) and location addresses for the detected particles. Data from each scan path is stored in memory. A three-dimensional surface map (95) is formed from the data stored in memory. The intensity traces for a particle (71) when combined together in the surface map form an intensity profile (97, 99, 101) or signature of the particle. These signatures may then be compared to known particle signatures to determine characteristics of the detected particle.
Abstract:
A single laser (30) is used to provide light for both dark (80) and bright field (60) detection. The laser beam is split into two beams by a Wollaston prism (40) and both beams are directed towards a sample (12) to be inspected to illuminate two areas (16, 18) of the sample. The light reflected by or transmitted through the sample at the two spots is then combined by the same or a different Wollaston prism and the phase shift caused by any anomaly of a sample is detected as a phase shift between the two beams by a bright field detector. Light scattered by the sample at the two spots is detected by a dark field detector. A halfwave plate (36) is used to orient the polarization plane of light from the laser incident on the Wollaston prism so that one of the two beams (52, 54) incident on the sample has a much higher intensity than the other and so that the sensitivity and the detection operation of dark field is not altered by the presence of two illuminated spots on the sample. A transparent dielectric at a suitable angle to the incident beam and the reflected or transmitted beam may be used to enhance bright field detection.
Abstract:
A light beam is directed towards a surface (12) along a direction normal to the surface (12). There is a scanning means (114, 116, 118) which causes the surface (12) to move so that the beam scans the surface (12) along a spiral path. Light scattered by the surface (12) within a first range of angles is collected by a first collection means (32, 34) and directed to a first detector (42), and light scattered within a second range is collected by a second collection means (38) and is directed to a second detector (44). The two ranges of collection angles are different, so that the first detector (42) is optimized to detect scattering from large particles, and the second detector (44) is optimized to detect light from small particles and defects.
Abstract:
An apparatus and method for inspecting a substrate (14), such as a semiconductor wafer, includes crossed cylindrical optical elements (44) that form an elliptical beam (40) that is caused to scan in parallel fashion at an oblique angle to the substrate (14). Preferably, the smaller dimension of the elliptical beam (40) is perpendicular to the direction of the scan of the beam across the wafer. A reflector (38) converts an angularly varying beam to a telecentrically scanning beam and also provides focusing only in the direction parallel to the telecentric scan.
Abstract:
An inspection apparatus for a light diffracting surface (w) employs a planar array of individually addressable light valves (69; 82; 84) for use as a spatial filter in an imaged Fourier plane of a diffraction pattern, with valves having stripe geometry (91; 93; 95) corresponding to positions of members (81; 83; 85) of the diffraction pattern, blocking light from those members. The remaining valve stripes, i.e. those not blocking light from diffraction order members, are open for transmission of light. Light (13; 31) directed onto the surface (w), such as a semiconductor wafer, forms elongated curved diffraction orders (65) from repetitive patterns of circuit features. The curved diffraction orders are transformed to linear orders by a Fourier transform lens (35a; 35b). The linear diffraction orders from repetitive patterns of circuit features are blocked, while light from non-repetitive features, such as dirt particles or defects, is allowed to pass through the light valves to a detector (47).