Hall sensor—magnet geometry for large stroke linear position sensing

Information

  • Patent Grant
  • 12247851
  • Patent Number
    12,247,851
  • Date Filed
    Thursday, February 29, 2024
    a year ago
  • Date Issued
    Tuesday, March 11, 2025
    2 months ago
Abstract
Position sensing units, comprising a magnetic assembly (MA) having a width W measured along a first direction and a height H measured along a second direction and including at least three magnets having respective magnetic polarizations that define along the first direction at least a left MA domain, a middle MA domain and a right MA domain, wherein the magnetic polarizations of each MA domain are different, and a magnetic flux measuring device (MFMD) for measuring a magnetic flux B, wherein the MA moves relative to the MFMD along the first direction within a stroke L that fulfils 1 mm≤L≤100 mm, stroke L beginning at a first point x0 and ending at a final point xmax, and wherein a minimum value Dmin of an orthogonal distance D, measured along the second direction between a particular MA domain and the MFMD, fulfills L/Dmin>10.
Description
FIELD

Embodiments disclosed herein relate in general to position sensing units, and in particular to position sensing in compact digital cameras included in mobile electronic devices.


BACKGROUND

Many compact digital cameras that are integrated in handheld electronic devices (“devices”) such as smartphones or tablets use actuators such as voice coil motors (VCMs) or stepper motors, e.g. for actuating a camera lens along a trajectory having a particular direction and range (“stroke” or “L”). The actuation is controlled by a position sensing unit, which is typically based on a magnet assembly (“MA”) that moves relative to a magnetic flux measuring device (MFMD) for example a Hall sensor. For stable control, the position sensing unit must support two conditions: a) it must exhibit linear behavior, i.e. its slope S=ΔB/Δx must be constant along the entire stroke (“linear range”), where ΔB is the change in magnetic flux density between two points located at a distance Δx from each other. For example, the linear range of the position sensing unit limits the stroke, and b) the slope S=ΔB/Δx within the linear range must be sufficiently steep, i.e. it must be above a certain threshold, e.g. S>50 mT or S>200 mT.



FIG. 1A shows a first known example of a position sensing unit 100 comprising a magnet assembly (“MA”) 102. MA 102 includes two rectangular magnets with a polarizations 104, the MA having a width W102 and a MA center “C” (with respect to the x direction or just “with respect to x”)) located at the symmetry axis (“SA”) 109 (with respect to the y direction or just “with respect to y”) of MA 102, and a MFMD 106. MA 102 causes a magnetic field 108 in its surroundings. MFMD 106 is located at a constant distance D=DC (measured along the y axis) from MA 102, which may be DC=0.1 mm-2 mm. For position sensing, MA 102 moves along a substantially straight line in the x direction and relative to MFMD 106. The position of MA 102 along the straight line (“x”) changes when x varies from x0 to xmax (this being the “stroke”). That is, MA moves within the stroke only. D is substantially constant between x0 and Xmas, i.e. D is not a function of x. In graph 107, the magnetic flux density (“B”) measured by MFMD 106 is shown versus the x position of MA 102. B is a function of x, i.e. B=B(x). Within stroke L ranging from x0 to xmax, slope S=(Bmax−B0)/L of B is linear. In some examples, W102 may be 0.6 mm-10 mm, L may be 0.5 mm-1 mm. In a typical example for focusing a camera lens, D=200 μm and L=700 μm, so that a ratio of L and D is L/D=3.5. For many actuator sensing examples, S is sufficiently steep. However, L/D is relatively small.



FIG. 1B shows a second known example of a position sensing unit 110 comprising a MA 112 that includes a single rectangular magnet having a polarization 114 and a width W112, and a MFMD 116. MA 112 causes a magnetic field 118. MFMD 116 is located at a distance D away from MA 102. Similar to the shown in FIG. 1A, a magnet center “C” (with respect to the x direction) is located at a SA 119 (with respect to the y direction) of MA 202. For position sensing, MA 112 moves along a substantially straight line in the x direction relative to MFMD 116. D is substantially constant between x0 and xmax. In graph 117, the magnetic flux density B measured by MFMD 116 is shown versus the x position of MA 112. Slope S=(Bmax−B0)/L of B is linear in a range L. L/D can be relatively large. However, for most actuator sensing scenarios, S is not sufficiently steep. Therefore, this design is hardly used in today's devices.


Novel Telephoto “(Tele”) cameras entering the market have large effective focal lengths (EFL) of e.g. 10 mm-40 mm for large zoom factors and for Macro photography with high object-to-image magnifications of e.g. 1:1-15:1 at object-lens distances (“u”) of 5 cm-15 cm. Focusing such a large EFL camera to a short u as small as 5 cm-15 cm requires large lens strokes significantly exceeding 1 mm.


Using the thin lens equation 1/EFL=1/u+1/v (“v” being the lens-image distance) and a Tele camera having EFL-25 mm as an example, a lens stroke of about 6.3 mm is required to focus to 10 cm (with respect to focus on infinity). Controlling such large lens strokes cannot be supported by position sensing units used at present in the compact camera industry. Further examples that require large strokes of components are, for example, (i) a 2-state zoom camera described in co-owned international patent application PCT/IB2020/051405, (ii) a pop out mechanism that collapses a camera's total track length (TTL) such as described in the co-owned international patent application PCT/IB2020/058697 and (iii) a continuous zoom camera such as described in co-owned U.S. provisional patent application No. 63/119,853 filed 1 Dec. 2020.


There is need for, and it would be beneficial to have a position sensing unit with a compact form factor that allows realizing position sensing with along large strokes L and with sufficiently large slope S.


SUMMARY

1. In various embodiments, there are provided position sensing units, comprising: a magnetic assembly (MA) having a width W measured along a first direction and a height H measured along a second direction and including at least three magnets having respective magnetic polarizations that define along the first direction at least a left MA domain, a middle MA domain and a right MA domain, wherein the magnetic polarizations of each MA domain are different; and a magnetic flux measuring device (MFMD) for measuring a magnetic flux B, wherein the MA is configured to move relative to the MFMD along the first direction within a stroke L that fulfils 1 mm≤L≤100 mm, stroke L beginning at a first point x0 and ending at a final point xmax, and wherein a minimum value Dmin of an orthogonal distance D measured along the second direction between a particular MA domain of the MA and the MFMD of the position sensing unit, fulfills L/Dmin>10. The magnets may be made from a Neodymium based material.


In some embodiments, the MA has a symmetry axis parallel to the second direction. In some embodiments, the symmetry axis is located at a center of the middle MA domain.


In some embodiments, D is not constant for different positions within stroke L.


In some embodiments, L/Dmin>15. In some embodiments, L/Dmin>20.


In some embodiments, B at x0 is B0 and B at xmax is Bmax, and a slope S=(B0−Bmax)/L is larger than 10 mT/mm. In some embodiments, S is larger than 100 mT/mm. In some embodiments, S is larger than 1000 mT/mm. In some embodiments, S is larger than 2500 mT/mm.


In some embodiments, the magnetic polarization of the left MA domain is directed towards the MFMD.


In some embodiments, the magnetic polarization of the right MA domain is directed away from the MFMD.


In some embodiments, the magnetic polarization of the middle MA domain is directed parallel or anti-parallel to the first direction.


In some embodiments, a position sensing unit as above or below may be included in a voice coil motor (VCM). In some embodiments, the VCM includes four coils. In some embodiments, the VCM is included in smartphone camera.


In some embodiments, the MFMD is a Hall sensor.


In some embodiments, a value of D between the left MA domain and MFMD is D(x0), wherein a value of D between the right MA domain and the MFMD is D(xmax), wherein a value of D between the middle MA domain and the MFMD is D(xmax/2) and wherein D(x0)≤D(xmax/2) and D(xmax)≤D(xmax/2). In some embodiments, a value of D between the middle MA domain and the MFMD is D(xmax/2) and wherein D(x0)=D(xmax)≤ D(xmax/2).


In some embodiments, the left, middle and right MA domains are rectangular. In some embodiments, the left and right MA domains are trapezoids, and the middle MA domain is a convex pentagon. In some embodiments, the left and right MA domains are trapezoids, and the middle MA domain is a concave pentagon.


In some embodiments, the MA additionally includes a fourth MA domain and a fifth MA domain having respective magnetic polarizations, wherein the fourth MA domain is located to the left of the left MA domain and wherein the fifth MA domain is located to the right of the right MA domain. In some embodiments, the magnetic polarization of the fourth MA domain is directed away from the MFMD. In some embodiments, the magnetic polarization of the fifth MA domain is directed towards the MFMD.


In some embodiments, L<20 mm. In some embodiments, L<10 mm. In some embodiments, L<7.5 mm. In some embodiments, L<5 mm.


In some embodiments, L/W>0.5. In some embodiments, L/W>0.75.


In some embodiments, L/H>3. In some embodiments, L/H>5.





BRIEF DESCRIPTION OF THE DRAWINGS

Non-limiting examples of embodiments disclosed herein are described below with reference to figures attached hereto that are listed following this paragraph. The drawings and descriptions are meant to illuminate and clarify embodiments disclosed herein, and should not be considered limiting in any way. Like elements in different drawings may be indicated like numerals.



FIG. 1A shows a first known example of a position sensing unit;



FIG. 1B shows a second known example of a position sensing unit;



FIG. 2A shows in cross-section an embodiment of a position sensing unit disclosed herein;



FIG. 2B shows a magnetic field distribution of a MA in the position sensing unit of FIG. 2A;



FIG. 2C shows the magnetic field density sensed by a MFMD in the position sensing unit of FIG. 2A;



FIG. 3 shows in cross-section another embodiment of a position sensing unit disclosed herein;



FIG. 4 shows in cross-section yet another embodiment of a position sensing unit disclosed herein;



FIG. 5A shows in cross-section yet another embodiment of a position sensing unit disclosed herein;



FIG. 5B shows an embodiment of a voice coil motor (“VCM”) disclosed herein.



FIG. 5C shows an embodiment of a camera including a lens assembly, a sensor, and a voice coil motor (VCM) including a position sensing unit attached to the lens assembly disclosed herein.





DETAILED DESCRIPTION


FIG. 2A shows an embodiment of a position sensing unit disclosed herein and numbered 200, comprising a magnet assembly 202 and a magnetic flux measuring device 206. Graph 207 shows B measured by MFMD 106 versus the x position of MA 102. FIG. 2B shows a magnetic field distribution 210 of MA 202. Box 212 indicates a y position within stroke L where a magnetic flux density 214 as shown in FIG. 2C is sensed by MFMD 206.


MA 202 includes three rectangular permanent magnets 202a, 202b and 202c having respective magnetic polarizations 204a, 204b and 204c. Magnets 202a and 202c are identical in shape and dimensions, but opposite respective magnetizations 204a and 204c. Magnets 202a and 202c are positioned symmetrically with respect to magnet 202b, i.e. both magnets 202a and 202c are (i) located at a same distance d202 from magnet 202b and (ii) are positioned at a same relative y coordinate ΔH with respect to magnet 202b. A center “C” of MA 202 is located at symmetry axis SA 209 of both magnet 202b and MA 202. MA 202 is shaped symmetrically around C with respect to y. MA 202 has a width W202 and a height H202.


Magnets described herein may be made from any material known to be used in the industry, specifically in digital cameras used in mobile electronic devices such as smartphones, for example any Neodymium based material, e.g. N48H, N48SH etc. x0 and xmax may be chosen so that their middle or symmetry point xS=xmax/2 is located at C, or they may be chosen otherwise. That is, the symmetry axis of the stroke with respect to y is located at xS=xmax/2 and may be identical with the SA 209 of MA 202 located at C (such as shown in FIG. 2A) or it may be located at another position.


The orthogonal distance between any component included in MA 202 and MFMD 206 is marked “D”. “Orthogonal distance” means that it represents only the y-component of a distance between any component included in MA 202 and MFMD 206. Values of D at points x0, C and xmax are marked respectively D(x0), DC and D(xmax). At x0 and Xmas, D has a minimal value Dmin.


As an example, D between magnet 202a and MFMD 206 is D(x0) and D between magnet 202b and MFMD 206 is DC, irrespective from the actual relative distance between magnet 202a and 202b respectively and MFMD 206. As to the relative motion of MA 202 and MFMD 206, in general an actual relative distance is composed of a distance component measured along x and a distance component measured along y. It is noted here that D refers to a distance between a magnet and a packaging device that includes a MFMD, and not to the distance the MFMD itself. In general, a MFMD is included in a packaging device having a housing, wherein the MFMD is located at a MFMD-housing distance of about 50 μm-250 μm from the housing. For calculating the distance between a magnet and the MFMD, the MFMD-housing distance must be added to D. Additionally, it is noted that D is not shown in scale.


In all examples shown herein, D(x0) and D(xmax) can be smaller than or equal to D(x) fulfilling D(x0), D(xmax)≤ D(x). The closest distance between one of the magnets and the MFMD Dmin=D(x0)=Dmax. That is, D(x0) and D(xmax) are smaller than or equal to all other distances in that range. In position sensing unit 200, D(x0)=D(xmax)<DC and L/Dmin>10. Typically, Dmin≥0.1 mm.


At x0, magnetic polarization 204a is directed substantially towards MFMD 206. At xmax, magnetic polarization 204c is directed substantially away from MFMD 206. At C, magnetic polarization 204b is directed substantially in parallel or anti-parallel to X. Magnets 202a, 202b and 202c define three MA domains, a left, a middle and a right MA domain respectively, wherein the magnet polarizations of each MA domain are different from each other.


Magnetic flux density B is a function of x, i.e. B=B(x). In L, the slope S=(Bmax−B0)/Ax of B is linear. In all following examples, S is given for an ideally linear slope such as 216 (see FIG. 2C) which has a same starting point (x0, B0) and a same end point (xmax, Bmax) as an actual slope 214 (see FIG. 2C). Values of S are given at DC.


As mentioned, graph 207 in FIG. 2C shows magnetic flux densities versus x, so it is a “B vs. x curve”. Actual magnetic flux density slope 214 is sensed along the coordinates indicated by the arrow L in FIG. 2A. Ideal (linear) magnetic flux density slope 216 is shown for comparison. Clearly, actual magnetic flux density slope 214 deviates from ideal magnetic flux density slope 216.



FIG. 3 shows another embodiment of a position sensing unit disclosed herein and numbered 300. Unit 300 comprises a MA 302 that includes three permanent magnets 302a, 302b and 302c having respective magnetic polarizations 304a, 304b and 304c, and a MFMD 306. Magnets 302a, 302b and 302c are not rectangular. Magnets 302a and 302c have identical shape and dimensions, but opposite magnetization 304a and 304c. Magnets 302a and 302c are positioned symmetrically with respect to 302b, i.e. both 302a and 302c are (i) located at a same distance d302 from 302b and (ii) are positioned at a same relative y coordinate ΔH302 with respect to 302b. Center C of MA 302 (with respect to x) is located at the SA 309 (with respect to y) of both magnet 302b and MA 302. MA 302 is shaped symmetrically around C with respect to y.


MA 302 causes a magnetic field (not shown). At C, MFMD 306 is located at DC away from MA 302. MA 302 moves along a stroke in x direction relative to MFMD 306. The position of MA 302 along x varies from x0 to xmax. x0 and xmax may be chosen so that their middle or symmetry point xs=xmax/2 is located at C, or they may be chosen otherwise. It is noted that D is not shown in scale.


Between x0 and xmax, orthogonal distance D is a function of x, D=D(x). For 300, D(x0)=D(xmax)<DC, D(x0)=D(xmax)=Dmin and L/Dmin≥10. Typically, Dmin≥0.1 mm. For the purpose of illustrating the definition of D, D is shown at 2 further, arbitrary positions x1 and x2, where D is given by D(x1) and D(x2) respectively. At x0, magnetic polarization 304a is substantially directed towards MFMD 306. At xmax, 304c is substantially directed away from MFMD 306. At C, 304b is directed substantially parallel or anti-parallel to x. Magnets 302a, 302b and 302c define three MA domains, a left, a middle and a right MA domain respectively, wherein the magnet polarizations of each MA domain are different from each other.


B 309 measured by MFMD 306 is shown versus the x position of MA 202 (“B versus x curve”). B is a function of x, i.e. B=B(x). In L, S=(Bmax−B0)/Δx of B is linear. Example values of given in Table 1. Values of S are given at DC. An advantage of MA 302 over MA 202 is that a B versus x curve within L exhibits a higher linearity. That is, the B vs. x curve of MA 302 varies less from an ideal linear shape such as 216 than the B vs. x curve of MA 202.












TABLE 1







Value
Unit



















W302
8
mm



H302
See HL302a




W302a
2.2
mm



HL302a
0.9




HR302a
0.55




W302b
2.7




H302b
0.6




d302
0.45




ΔH302b
0.1




S
 10-6000
mT/mm, at DC.



L
7.5
mm



DC
0.2-1  
mm



Dmin
0.1-0.7
mm



L/W302
0.94




L/H302
8.33




HL302a/HR302a
1.64




H302b/ΔH302b
6




L/Dmin
10.7-75  











FIG. 4 shows yet another embodiment of a position sensing unit disclosed herein and numbered 400. Unit 400 comprises a MA 402 that includes three non-rectangular permanent magnets 402a, 402b and 402c having respective magnetic polarization 404a, 404b and 404c, and a MFMD 406. Magnets 402a and 402c have the same shape and dimensions, but opposite magnetizations 404a and 404c. Magnets 402a and 402c are positioned symmetrically with respect to 402b, i.e. both 402a and 402c are (i) located at a same distance d402 from 402b and (ii) are positioned at a same relative Y coordinate ΔH402 with respect to 402b. Center C of MA 402 (with respect to x) is located at the SA 409 (with respect to y) of both magnet 402b and MA 402. MA 402 is shaped symmetrically around C with respect to y.


MA 402 causes a magnetic field (not shown). At C. MFMD 406 is located at DC away from MA 402. MA 402 moves along a stroke in x direction relative to MFMD 406. The position of MA 402 along x varies from x0 to xmax. x0 and xmax may be chosen so that their middle or symmetry point xs=xmax/2 is located at C, or they may be chosen otherwise.


Between x0 to xmax, orthogonal distance D is a function of x, D=D(x). For 400, D(x0)=D(xmax)<DC, D(x0)=D(xmax)=Dmin and L/Dmin>10. Typically, Dmin≥0.1 mm. At x0, the magnetic polarization 404a is substantially directed towards MFMD 406. At xmax, 404c is substantially directed away from MFMD 406. At C, 404b is directed substantially parallel or anti-parallel to X. Magnets 402a, 402b and 402c define three MA domains, a left, a middle and a right MA domain respectively, wherein the magnet polarizations of each MA domain are different from each other. It is noted that D is not shown in scale.


B 409 measured by MFMD 406 is shown versus the x position of MA 202. B is a function of x, i.e. B=B(x). In L, S=(Bmax−B0)/ΔX of B is linear. Example values of position sensing unit 400 are given in Table 2. Values of S are given at DC. An advantage of MA 402 over MA 202 is that a B versus x curve within L exhibits a higher linearity.











TABLE 2






Value
Unit

















W402
5.35



H402
See HL402a



W402a
1.55



HL402a
0.8



HR402a
0.55



WR402a
0.625



W402b
1.2



H402b
0.55



d402
0.525



ΔH402b
0.05



S
 10-6000
mT/mm, at DC.


L
5
mm


Dmin
0.1-0.5
mm


DC
0.2-1  
mm


L/W402
0.93



L/H402
6.25



HL402a/HR402a
1.45



H402b/ΔH402b
11



L/Dmin
10.0-50  











FIG. 5A shows yet another embodiment of a position sensing unit disclosed herein and numbered 500. Unit 500 comprises a MA 502 that includes five permanent magnets 502a, 502b, 502c, 502d and 502e having respective magnetic polarizations 504a, 504b, 504c, 504d and 504e, and a MFMD 506. Magnets 502a, 502b and 502c are not rectangular, while magnets 502d and 502e are rectangular. Magnets 502a and 502c as well as 502d and 502e have the same shape and dimensions, but opposite magnetizations 504a and 504c and 504d and 504e respectively. Magnets 502a, 502c, 502d and 502e are positioned symmetrically with respect to magnet 502b. A magnet sub-assembly including magnets 502a, 502b and 502c is identical with MA 302 shown in FIG. 3. Center C of MA 502 (with respect to x) is located at the SA 509 (with respect to y) of both magnet 502b and MA 502. MA 502 is shaped symmetrically around C with respect to y.


MA 502 causes a magnetic field (not shown). At C, MFMD 506 is located at De away from MA 502. MA 502 moves along a stroke in x direction relative to MFMD 506. The position of MA 502 along x varies from x0 to xmax. x0 and xmax may be chosen so that their middle or symmetry point xs=xmax/2 is located at C, or they may be chosen otherwise.


Between x0 to xmax, orthogonal distance D is a function of x, D=D(x). For 500, D(x0)=D(xmax)<DC, D(x0)=D(xmax)=Dmin and L/Dmin>10. Typically, Dmin≥0.1 mm. At x0, the magnetic polarization 504a is substantially directed towards MFMD 506. At xmax, 504c is substantially directed away from MFMD 506. At C, 504b is directed substantially parallel or anti-parallel to X. 504d is directed substantially anti-parallel to 504a. 504e is directed substantially anti-parallel to 504c. Additionally to the three MA domains defined by magnets 502a, 502b and 502c, in MA 502 there are two additional MA domains defined by magnets 502d and 502e.


B (not shown) is measured by MFMD 506 versus the x position of MA 202. B is a function of x, i.e. B=B(x). In L, S=(Bmax−B0)/ΔX of B is linear. Example values of given in Table 3. For the values of magnet sub-assembly including magnets 502a, 502b and 502c see magnets 302a, 302b and 302c of Table 1 respectively. Values of S are given at DC.


An advantage of MA 502 over MA 302 is that a B versus x curve has a higher linearity for the same dimensions of magnets 502a, 502b and 502c (which have the same dimensions as magnets 302a, 302b and 302c).











TABLE 3






Value
Unit

















W502
19.2
mm


H502
See H502d
mm


W502d, W502e
2.55
mm


H502d, H502e
0.9
mm


S
 10-6000
mT/mm, at DC.


L
13.4
mm


Dmin
0.1-1  
mm


DC
0.2-0.9
mm


L/W502
0.70



L/H502
14.89



L/Dmin
13.4-134 











FIG. 5B shows an embodiment of a voice coil motor (“VCM”) disclosed herein and numbered 510. VCM 510 includes a coil assembly (“CA”) 520 and position sensing unit 500. CA 520 includes four coils 520a, 520b, 520c and 520d and can generate a magnetic field.


In VCM 510, the magnetic field caused by position sensing unit 500 additionally provides, together with the magnetic field generated by CA 520, the magnetic field configuration which is required for actuating a relative motion between MA 502 and CA 520 as well as MFMD 506. Typically and with respect to a device that includes VCM 510, MFMD 506 and CA 520 are at rest and MA 502 moves. In some examples for lens focusing in devices that include a camera, as shown in exemplary FIG. 5C. MA 502 may be fixedly coupled to a camera's lens (LENS) 550 for actuating the lens with respect to camera's image sensor (SNS) 552 which is at rest with respect to the device. An advantage of MA 502 over MA 302 is that it allows a faster VCM actuation.

    • In other embodiments, a VCM like VCM 510 may include position sensing unit 200, 300 or 400.


While this disclosure has been described in terms of certain embodiments and generally associated methods, alterations and permutations of the embodiments and methods will be apparent to those skilled in the art. The disclosure is to be understood as not limited by the specific embodiments described herein, but only by the scope of the appended claims.


Unless otherwise stated, the use of the expression “and/or” between the last two members of a list of options for selection indicates that a selection of one or more of the listed options is appropriate and may be made.


It should be understood that where the claims or specification refer to “a” or “an” element, such reference is not to be construed as there being only one of that element.


Furthermore, for the sake of clarity the term “substantially” is used herein to imply the possibility of variations in values within an acceptable range. According to one example, the term “substantially” used herein should be interpreted to imply possible variation of up to 10% over or under any specified value. According to another example, the term “substantially” used herein should be interpreted to imply possible variation of up to 5% over or under any specified value. According to a further example, the term “substantially” used herein should be interpreted to imply possible variation of up to 2.5% over or under any specified value.


All references mentioned in this specification are herein incorporated in their entirety by reference into the specification, to the same extent as if each individual reference was specifically and individually indicated to be incorporated herein by reference. In addition, citation or identification of any reference in this application shall not be construed as an admission that such reference is available as prior art to the present invention.

Claims
  • 1. A camera, comprising: a lens;a stationary image sensor;a magnetic assembly (MA) fixedly coupled to the lens and having a width W measured along a first direction associated with a direction of actuation of the lens relative to the stationary sensor, and a height H measured along a second direction that is perpendicular to the first direction, the MA including at least three magnets having respective magnetic polarizations that define along the first direction at least a left MA domain, a middle MA domain and a right MA domain, wherein the magnetic polarizations of each of the MA domains are different; anda stationary magnetic flux measuring device (MFMD) for measuring a magnetic flux B, wherein the MA is configured to move relative to the MFMD along the first direction within a range defined by a stroke L that fulfils 1 mm≤L≤100 mm,wherein a minimum value Dmin of an orthogonal distance D measured along the second direction between a particular magnet and the MFMD of the position sensing unit fulfills L/Dmin>10,wherein the at least three magnets are positioned sequentially along the first direction,and wherein adjacent magnets are separated by a gap.
  • 2. The camera of claim 1, wherein the lens has an effective focal length EFL in the range of 10 mm to 40 mm.
  • 3. The camera of claim 1, wherein the MA has a symmetry axis parallel to the second direction.
  • 4. The camera of claim 1, wherein D is not constant for different positions within stroke L.
  • 5. The camera of claim 1, wherein the magnetic polarization of the left MA domain is directed towards the MFMD and the magnetic polarization of the right MA domain is directed away from the MFMD.
  • 6. The camera of claim 1, wherein the magnetic polarization of the middle MA domain is directed parallel or anti-parallel to the first direction.
  • 7. The camera of claim 1, wherein the left, middle and right MA domains are rectangular.
  • 8. The camera of claim 1, wherein the left and right MA domains are trapezoids, and the middle MA domain is a pentagon.
  • 9. The camera of claim 1, wherein the MA includes a fourth MA domain and a fifth MA domain having respective magnetic polarizations, wherein the fourth MA domain is located to the left of the left MA domain and wherein the fifth MA domain is located to the right of the right MA domain.
  • 10. The camera of claim 1, wherein L<20 mm.
  • 11. The camera of claim 1, wherein L<5 mm.
  • 12. The camera of claim 1, wherein L/W>0.5.
  • 13. The camera of claim 1, wherein L/H>5.
  • 14. The camera of claim 1, wherein L/Dmin>15.
  • 15. The camera of claim 1, wherein stroke L starts at a first point x0 and ends at a final point xmax, wherein a value of D between the left magnet and MFMD is D(x0), wherein a value of D between the right magnet and the MFMD is D(xmax), wherein a value of D between the middle magnet and the MFMD is D(xmax/2) and wherein D(x0)≤D(xmax/2) and D(xmax)≤D(xmax/2).
  • 16. The camera of claim 1, wherein stroke L starts at a first point x0 and ends at a final point xmax, wherein a value of D between the left magnet and MFMD is D(x), wherein a value of D between the right magnet and the MFMD is D(xmax), wherein a value of D between the middle magnet and the MFMD is D(xmax/2) and wherein D(x0)=D(xmax)≤D(xmax/2).
  • 17. The camera of claim 1, wherein the MA and the MFMD are included in a voice coil motor (VCM).
  • 18. The camera of claim 17, wherein the VCM includes four coils.
  • 19. The camera of claim 1, wherein the camera is included in a mobile device.
  • 20. The camera of claim 19, wherein the mobile device is a smartphone.
CROSS REFERENCE TO EXISTING APPLICATIONS

This application is a continuation from U.S. patent application Ser. No. 17/628,905 filed Jan. 21, 2022 (now allowed), which was a 371 of international patent application PCT/IB2021/056693 filed Jul. 26, 2021, and claims priority from U.S. Provisional Patent Application No. 63/059,200 filed Jul. 31, 2020, which is incorporated herein by reference in its entirety.

US Referenced Citations (399)
Number Name Date Kind
3085354 Rasmussen et al. Apr 1963 A
3584513 Gates Jun 1971 A
3941001 LaSarge Mar 1976 A
4199785 McCullough et al. Apr 1980 A
4792822 Akiyama et al. Dec 1988 A
5005083 Grage et al. Apr 1991 A
5032917 Aschwanden Jul 1991 A
5041852 Misawa et al. Aug 1991 A
5051830 von Hoessle Sep 1991 A
5099263 Matsumoto et al. Mar 1992 A
5248971 Mandl Sep 1993 A
5287093 Amano et al. Feb 1994 A
5331465 Miyano Jul 1994 A
5394520 Hall Feb 1995 A
5436660 Sakamoto Jul 1995 A
5444478 Lelong et al. Aug 1995 A
5459520 Sasaki Oct 1995 A
5502537 Utagawa Mar 1996 A
5657402 Bender et al. Aug 1997 A
5682198 Katayama et al. Oct 1997 A
5768443 Michael et al. Jun 1998 A
5892855 Kakinami et al. Apr 1999 A
5926190 Turkowski et al. Jul 1999 A
5940641 McIntyre et al. Aug 1999 A
5982951 Katayama et al. Nov 1999 A
6101334 Fantone Aug 2000 A
6128416 Oura Oct 2000 A
6148120 Sussman Nov 2000 A
6201533 Rosenberg et al. Mar 2001 B1
6208765 Bergen Mar 2001 B1
6211668 Duesler et al. Apr 2001 B1
6215299 Reynolds et al. Apr 2001 B1
6222359 Duesler et al. Apr 2001 B1
6268611 Pettersson et al. Jul 2001 B1
6520643 Holman et al. Feb 2003 B1
6549215 Jouppi Apr 2003 B2
6611289 Yu et al. Aug 2003 B1
6643416 Daniels et al. Nov 2003 B1
6650368 Doron Nov 2003 B1
6680748 Monti Jan 2004 B1
6714665 Hanna et al. Mar 2004 B1
6724421 Glatt Apr 2004 B1
6738073 Park et al. May 2004 B2
6741250 Furlan et al. May 2004 B1
6750903 Miyatake et al. Jun 2004 B1
6778207 Lee et al. Aug 2004 B1
7002583 Rabb, III Feb 2006 B2
7015954 Foote et al. Mar 2006 B1
7038716 Klein et al. May 2006 B2
7199348 Olsen et al. Apr 2007 B2
7206136 Labaziewicz et al. Apr 2007 B2
7248294 Slatter Jul 2007 B2
7256944 Labaziewicz et al. Aug 2007 B2
7305180 Labaziewicz et al. Dec 2007 B2
7339621 Fortier Mar 2008 B2
7346217 Gold, Jr. Mar 2008 B1
7365793 Cheatle et al. Apr 2008 B2
7411610 Doyle Aug 2008 B2
7424218 Baudisch et al. Sep 2008 B2
7509041 Hosono Mar 2009 B2
7533819 Barkan et al. May 2009 B2
7619683 Davis Nov 2009 B2
7738016 Toyofuku Jun 2010 B2
7773121 Huntsberger et al. Aug 2010 B1
7809256 Kuroda et al. Oct 2010 B2
7880776 LeGall et al. Feb 2011 B2
7918398 Li et al. Apr 2011 B2
7964835 Olsen et al. Jun 2011 B2
7978239 Deever et al. Jul 2011 B2
8115825 Culbert et al. Feb 2012 B2
8149327 Lin et al. Apr 2012 B2
8154610 Jo et al. Apr 2012 B2
8238695 Davey et al. Aug 2012 B1
8274552 Dahi et al. Sep 2012 B2
8390729 Long et al. Mar 2013 B2
8391697 Cho et al. Mar 2013 B2
8400555 Georgiev et al. Mar 2013 B1
8439265 Ferren et al. May 2013 B2
8446484 Muukki et al. May 2013 B2
8483452 Ueda et al. Jul 2013 B2
8514491 Duparre Aug 2013 B2
8547389 Hoppe et al. Oct 2013 B2
8553106 Scarff Oct 2013 B2
8587691 Takane Nov 2013 B2
8619148 Watts et al. Dec 2013 B1
8752969 Kane et al. Jun 2014 B1
8803990 Smith Aug 2014 B2
8896655 Mauchly et al. Nov 2014 B2
8976255 Matsuoto et al. Mar 2015 B2
9019387 Nakano Apr 2015 B2
9025073 Attar et al. May 2015 B2
9025077 Attar et al. May 2015 B2
9041835 Honda May 2015 B2
9137447 Shibuno Sep 2015 B2
9185291 Shabtay et al. Nov 2015 B1
9215377 Sokeila et al. Dec 2015 B2
9215385 Luo Dec 2015 B2
9270875 Brisedoux et al. Feb 2016 B2
9286680 Jiang et al. Mar 2016 B1
9344626 Silverstein et al. May 2016 B2
9360671 Zhou Jun 2016 B1
9369621 Malone et al. Jun 2016 B2
9413930 Geerds Aug 2016 B2
9413984 Attar et al. Aug 2016 B2
9420180 Jin Aug 2016 B2
9438792 Nakada et al. Sep 2016 B2
9485432 Medasani et al. Nov 2016 B1
9578257 Attar et al. Feb 2017 B2
9618748 Munger et al. Apr 2017 B2
9681057 Attar et al. Jun 2017 B2
9723220 Sugie Aug 2017 B2
9736365 Laroia Aug 2017 B2
9736391 Du et al. Aug 2017 B2
9768310 Ahn et al. Sep 2017 B2
9800798 Ravirala et al. Oct 2017 B2
9851803 Fisher et al. Dec 2017 B2
9894287 Qian et al. Feb 2018 B2
9900522 Lu Feb 2018 B2
9927600 Goldenberg et al. Mar 2018 B2
11700441 Shahparnia Jul 2023 B1
11946775 Kowal Apr 2024 B2
20020005902 Yuen Jan 2002 A1
20020030163 Zhang Mar 2002 A1
20020054214 Yoshikawa May 2002 A1
20020063711 Park et al. May 2002 A1
20020075258 Park et al. Jun 2002 A1
20020122113 Foote Sep 2002 A1
20020136554 Nomura et al. Sep 2002 A1
20020167741 Koiwai et al. Nov 2002 A1
20030030729 Prentice et al. Feb 2003 A1
20030093805 Gin May 2003 A1
20030156751 Lee et al. Aug 2003 A1
20030160886 Misawa et al. Aug 2003 A1
20030162564 Kimura et al. Aug 2003 A1
20030202113 Yoshikawa Oct 2003 A1
20040008773 Itokawa Jan 2004 A1
20040012683 Yamasaki et al. Jan 2004 A1
20040017386 Liu et al. Jan 2004 A1
20040027367 Pilu Feb 2004 A1
20040061788 Bateman Apr 2004 A1
20040141065 Hara et al. Jul 2004 A1
20040141086 Mihara Jul 2004 A1
20040227838 Atarashi et al. Nov 2004 A1
20040239313 Godkin Dec 2004 A1
20040240052 Minefuji et al. Dec 2004 A1
20050013509 Samadani Jan 2005 A1
20050046740 Davis Mar 2005 A1
20050134697 Mikkonen et al. Jun 2005 A1
20050141390 Lee et al. Jun 2005 A1
20050157184 Nakanishi et al. Jul 2005 A1
20050168834 Matsumoto et al. Aug 2005 A1
20050185049 Iwai et al. Aug 2005 A1
20050200718 Lee Sep 2005 A1
20050248667 Schweng et al. Nov 2005 A1
20060054782 Olsen et al. Mar 2006 A1
20060056056 Ahiska et al. Mar 2006 A1
20060067672 Washisu et al. Mar 2006 A1
20060102907 Lee et al. May 2006 A1
20060125937 LeGall et al. Jun 2006 A1
20060126737 Boice et al. Jun 2006 A1
20060170793 Pasquarette et al. Aug 2006 A1
20060175549 Miller et al. Aug 2006 A1
20060181619 Liow et al. Aug 2006 A1
20060187310 Janson et al. Aug 2006 A1
20060187322 Janson et al. Aug 2006 A1
20060187338 May et al. Aug 2006 A1
20060227236 Pak Oct 2006 A1
20070024737 Nakamura et al. Feb 2007 A1
20070114990 Godkin May 2007 A1
20070126911 Nanjo Jun 2007 A1
20070127040 Davidovici Jun 2007 A1
20070159344 Kisacanin Jul 2007 A1
20070177025 Kopet et al. Aug 2007 A1
20070188653 Pollock et al. Aug 2007 A1
20070189386 Imagawa et al. Aug 2007 A1
20070257184 Olsen et al. Nov 2007 A1
20070285550 Son Dec 2007 A1
20080017557 Witdouck Jan 2008 A1
20080024614 Li et al. Jan 2008 A1
20080025634 Border et al. Jan 2008 A1
20080030592 Border et al. Feb 2008 A1
20080030611 Jenkins Feb 2008 A1
20080084484 Ochi et al. Apr 2008 A1
20080088942 Seo Apr 2008 A1
20080106629 Kurtz et al. May 2008 A1
20080117316 Orimoto May 2008 A1
20080129831 Cho et al. Jun 2008 A1
20080218611 Parulski et al. Sep 2008 A1
20080218612 Border et al. Sep 2008 A1
20080218613 Janson et al. Sep 2008 A1
20080219654 Border et al. Sep 2008 A1
20090086074 Li et al. Apr 2009 A1
20090102948 Scherling Apr 2009 A1
20090109556 Shimizu et al. Apr 2009 A1
20090122195 Van Baar et al. May 2009 A1
20090122406 Rouvinen et al. May 2009 A1
20090128644 Camp et al. May 2009 A1
20090168135 Yu et al. Jul 2009 A1
20090200451 Conners Aug 2009 A1
20090219547 Kauhanen et al. Sep 2009 A1
20090234542 Orlewski Sep 2009 A1
20090252484 Hasuda et al. Oct 2009 A1
20090295949 Ojala Dec 2009 A1
20090295986 Topliss et al. Dec 2009 A1
20090324135 Kondo et al. Dec 2009 A1
20100013906 Border et al. Jan 2010 A1
20100020221 Tupman et al. Jan 2010 A1
20100060746 Olsen et al. Mar 2010 A9
20100097444 Lablans Apr 2010 A1
20100103194 Chen et al. Apr 2010 A1
20100134621 Namkoong et al. Jun 2010 A1
20100165131 Makimoto et al. Jul 2010 A1
20100196001 Ryynänen et al. Aug 2010 A1
20100202068 Ito Aug 2010 A1
20100238327 Griffith et al. Sep 2010 A1
20100246024 Aoki et al. Sep 2010 A1
20100259836 Kang et al. Oct 2010 A1
20100265331 Tanaka Oct 2010 A1
20100283842 Guissin et al. Nov 2010 A1
20100321494 Peterson et al. Dec 2010 A1
20110043193 Aebi et al. Feb 2011 A1
20110058320 Kim et al. Mar 2011 A1
20110063417 Peters et al. Mar 2011 A1
20110063446 McMordie et al. Mar 2011 A1
20110064327 Dagher et al. Mar 2011 A1
20110080487 Venkataraman et al. Apr 2011 A1
20110121666 Park et al. May 2011 A1
20110128288 Petrou et al. Jun 2011 A1
20110164172 Shintani et al. Jul 2011 A1
20110221599 Högasten Sep 2011 A1
20110229054 Weston et al. Sep 2011 A1
20110234798 Chou Sep 2011 A1
20110234853 Hayashi et al. Sep 2011 A1
20110234881 Wakabayashi et al. Sep 2011 A1
20110242286 Pace et al. Oct 2011 A1
20110242355 Goma et al. Oct 2011 A1
20110285714 Swic et al. Nov 2011 A1
20110298966 Kirschstein et al. Dec 2011 A1
20120014682 David et al. Jan 2012 A1
20120026366 Golan et al. Feb 2012 A1
20120044372 Cote et al. Feb 2012 A1
20120062780 Morihisa Mar 2012 A1
20120069235 Imai Mar 2012 A1
20120075489 Nishihara Mar 2012 A1
20120105579 Jeon et al. May 2012 A1
20120124525 Kang May 2012 A1
20120154547 Aizawa Jun 2012 A1
20120154614 Moriya et al. Jun 2012 A1
20120196648 Havens et al. Aug 2012 A1
20120229663 Nelson et al. Sep 2012 A1
20120249815 Bohn et al. Oct 2012 A1
20120287315 Huang et al. Nov 2012 A1
20120320467 Baik et al. Dec 2012 A1
20130002928 Imai Jan 2013 A1
20130016427 Sugawara Jan 2013 A1
20130063629 Webster et al. Mar 2013 A1
20130076922 Shihoh et al. Mar 2013 A1
20130093842 Yahata Apr 2013 A1
20130094126 Rappoport et al. Apr 2013 A1
20130113894 Mirlay May 2013 A1
20130135445 Dahi et al. May 2013 A1
20130148215 Mori et al. Jun 2013 A1
20130148854 Wang et al. Jun 2013 A1
20130155176 Paripally et al. Jun 2013 A1
20130163085 Lim et al. Jun 2013 A1
20130182150 Asakura Jul 2013 A1
20130201360 Song Aug 2013 A1
20130202273 Ouedraogo et al. Aug 2013 A1
20130229544 Bando Sep 2013 A1
20130235224 Park et al. Sep 2013 A1
20130250150 Malone et al. Sep 2013 A1
20130258044 Betts-LaCroix Oct 2013 A1
20130258048 Wang et al. Oct 2013 A1
20130270419 Singh et al. Oct 2013 A1
20130278785 Nomura et al. Oct 2013 A1
20130286221 Shechtman et al. Oct 2013 A1
20130321668 Kamath Dec 2013 A1
20140009631 Topliss Jan 2014 A1
20140049615 Uwagawa Feb 2014 A1
20140118584 Lee et al. May 2014 A1
20140160311 Hwang et al. Jun 2014 A1
20140192224 Laroia Jul 2014 A1
20140192238 Attar et al. Jul 2014 A1
20140192253 Laroia Jul 2014 A1
20140218587 Shah Aug 2014 A1
20140313316 Olsson et al. Oct 2014 A1
20140362242 Takizawa Dec 2014 A1
20140376090 Terajima Dec 2014 A1
20140379103 Ishikawa et al. Dec 2014 A1
20150002683 Hu et al. Jan 2015 A1
20150002684 Kuchiki Jan 2015 A1
20150042870 Chan et al. Feb 2015 A1
20150070781 Cheng et al. Mar 2015 A1
20150086127 Camilus et al. Mar 2015 A1
20150092066 Geiss et al. Apr 2015 A1
20150103147 Ho et al. Apr 2015 A1
20150110345 Weichselbaum Apr 2015 A1
20150124059 Georgiev et al. May 2015 A1
20150138381 Ahn May 2015 A1
20150145965 Livyatan et al. May 2015 A1
20150154776 Zhang et al. Jun 2015 A1
20150162048 Hirata et al. Jun 2015 A1
20150181115 Mashiah Jun 2015 A1
20150195458 Nakayama et al. Jul 2015 A1
20150198464 El Alami Jul 2015 A1
20150215516 Dolgin Jul 2015 A1
20150237280 Choi et al. Aug 2015 A1
20150242994 Shen Aug 2015 A1
20150244906 Wu et al. Aug 2015 A1
20150253543 Mercado Sep 2015 A1
20150253647 Mercado Sep 2015 A1
20150261299 Wajs Sep 2015 A1
20150271471 Hsieh et al. Sep 2015 A1
20150281678 Park et al. Oct 2015 A1
20150286033 Osborne Oct 2015 A1
20150296112 Park et al. Oct 2015 A1
20150316744 Chen Nov 2015 A1
20150334309 Peng et al. Nov 2015 A1
20160028949 Lee et al. Jan 2016 A1
20160044250 Shabtay et al. Feb 2016 A1
20160070088 Koguchi Mar 2016 A1
20160154066 Hioka et al. Jun 2016 A1
20160154202 Wippermann et al. Jun 2016 A1
20160154204 Lim et al. Jun 2016 A1
20160212358 Shikata Jul 2016 A1
20160212418 Demirdjian et al. Jul 2016 A1
20160238834 Erlich et al. Aug 2016 A1
20160241751 Park Aug 2016 A1
20160245669 Nomura Aug 2016 A1
20160291295 Shabtay et al. Oct 2016 A1
20160295112 Georgiev et al. Oct 2016 A1
20160301840 Du et al. Oct 2016 A1
20160301868 Acharya et al. Oct 2016 A1
20160342095 Bieling et al. Nov 2016 A1
20160353008 Osborne Dec 2016 A1
20160353012 Kao et al. Dec 2016 A1
20160381289 Kim et al. Dec 2016 A1
20170001577 Seagraves et al. Jan 2017 A1
20170019616 Zhu et al. Jan 2017 A1
20170070731 Darling et al. Mar 2017 A1
20170094187 Sharma et al. Mar 2017 A1
20170124987 Kim et al. May 2017 A1
20170150061 Shabtay et al. May 2017 A1
20170187962 Lee et al. Jun 2017 A1
20170214846 Du et al. Jul 2017 A1
20170214866 Zhu et al. Jul 2017 A1
20170219749 Hou et al. Aug 2017 A1
20170242225 Fiske Aug 2017 A1
20170276954 Bajorins et al. Sep 2017 A1
20170289458 Song et al. Oct 2017 A1
20180003925 Shmunk Jan 2018 A1
20180013944 Evans, V et al. Jan 2018 A1
20180017844 Yu et al. Jan 2018 A1
20180024329 Goldenberg et al. Jan 2018 A1
20180059379 Chou Mar 2018 A1
20180109660 Yoon et al. Apr 2018 A1
20180109710 Lee et al. Apr 2018 A1
20180120674 Avivi et al. May 2018 A1
20180150973 Tang et al. May 2018 A1
20180176426 Wei et al. Jun 2018 A1
20180184010 Cohen et al. Jun 2018 A1
20180198897 Tang et al. Jul 2018 A1
20180216925 Yasuda et al. Aug 2018 A1
20180241922 Baldwin et al. Aug 2018 A1
20180249090 Nakagawa et al. Aug 2018 A1
20180295292 Lee et al. Oct 2018 A1
20180300901 Wakai et al. Oct 2018 A1
20180307005 Price et al. Oct 2018 A1
20180329281 Ye Nov 2018 A1
20180368656 Austin et al. Dec 2018 A1
20190089941 Bigioi et al. Mar 2019 A1
20190096047 Ogasawara Mar 2019 A1
20190100156 Chung et al. Apr 2019 A1
20190121103 Bachar et al. Apr 2019 A1
20190121216 Shabtay et al. Apr 2019 A1
20190130822 Jung et al. May 2019 A1
20190154466 Fletcher May 2019 A1
20190213712 Lashdan et al. Jul 2019 A1
20190215440 Rivard et al. Jul 2019 A1
20190222758 Goldenberg et al. Jul 2019 A1
20190227338 Bachar et al. Jul 2019 A1
20190228562 Song Jul 2019 A1
20190297238 Klosterman Sep 2019 A1
20190320119 Miyoshi Oct 2019 A1
20200014912 Kytsun et al. Jan 2020 A1
20200092486 Guo et al. Mar 2020 A1
20200103726 Shabtay et al. Apr 2020 A1
20200104034 Lee et al. Apr 2020 A1
20200118287 Hsieh et al. Apr 2020 A1
20200134848 El-Khamy et al. Apr 2020 A1
20200162682 Cheng et al. May 2020 A1
20200221026 Fridman et al. Jul 2020 A1
20200264403 Bachar et al. Aug 2020 A1
20200389580 Kodama et al. Dec 2020 A1
20210180989 Fukumura et al. Jun 2021 A1
20210208415 Goldenberg et al. Jul 2021 A1
20210333521 Yedid et al. Oct 2021 A9
20220252963 Shabtay et al. Aug 2022 A1
20220368814 Topliss et al. Nov 2022 A1
Foreign Referenced Citations (75)
Number Date Country
101276415 Oct 2008 CN
201514511 Jun 2010 CN
102130567 Jul 2011 CN
102215373 Oct 2011 CN
102739949 Oct 2012 CN
102982518 Mar 2013 CN
103024272 Apr 2013 CN
203406908 Jan 2014 CN
103841404 Jun 2014 CN
205301703 Jun 2016 CN
105827903 Aug 2016 CN
105847662 Aug 2016 CN
107608052 Jan 2018 CN
107682489 Feb 2018 CN
109729266 May 2019 CN
1536633 Jun 2005 EP
1780567 May 2007 EP
2523450 Nov 2012 EP
S59191146 Oct 1984 JP
04211230 Aug 1992 JP
H07318864 Dec 1995 JP
08271976 Oct 1996 JP
2002010276 Jan 2002 JP
2003298920 Oct 2003 JP
2003304024 Oct 2003 JP
2004056779 Feb 2004 JP
2004133054 Apr 2004 JP
2004245982 Sep 2004 JP
2005099265 Apr 2005 JP
2005122084 May 2005 JP
2005321592 Nov 2005 JP
2006038891 Feb 2006 JP
2006191411 Jul 2006 JP
2006237914 Sep 2006 JP
2006238325 Sep 2006 JP
2008083377 Sep 2006 JP
2007228006 Sep 2007 JP
2007306282 Nov 2007 JP
2008076485 Apr 2008 JP
2008245142 Oct 2008 JP
2008271026 Nov 2008 JP
2010204341 Sep 2010 JP
2011055246 Mar 2011 JP
2011085666 Apr 2011 JP
2011138407 Jul 2011 JP
2011203283 Oct 2011 JP
2012132739 Jul 2012 JP
2013101213 May 2013 JP
2013106289 May 2013 JP
2016105577 Jun 2016 JP
2017146440 Aug 2017 JP
2019126179 Jul 2019 JP
20070005946 Jan 2007 KR
20090058229 Jun 2009 KR
20100008936 Jan 2010 KR
20110080590 Jul 2011 KR
20130104764 Sep 2013 KR
1020130135805 Nov 2013 KR
20140014787 Feb 2014 KR
101428042 Aug 2014 KR
101477178 Dec 2014 KR
20140144126 Dec 2014 KR
20150118012 Oct 2015 KR
20170105236 Sep 2017 KR
20180120894 Nov 2018 KR
20130085116 Jun 2019 KR
I407177 Sep 2013 TW
2000027131 May 2000 WO
2004084542 Sep 2004 WO
2006008805 Jan 2006 WO
2010122841 Oct 2010 WO
2014072818 May 2014 WO
2017025822 Feb 2017 WO
2017037688 Mar 2017 WO
2018130898 Jul 2018 WO
Non-Patent Literature Citations (18)
Entry
Zitova Bet al: “Image Registration Methods: a Survey”, Image and Vision Computing, Elsevier, Guildford, GB, vol. 21, No. 11, Oct. 1, 2003 (Oct. 1, 2003), pp. 977-1000, XP00i 189327, ISSN: 0262-8856, DOI: 10_i0i6/ S0262-8856(03)00137-9.
Office Action in related CN patent application 202180005008.5, dated Oct. 28, 2023.
Statistical Modeling and Performance Characterization of a Real-Time Dual Camera Surveillance System, Greienhagen et al., Publisher: IEEE, 2000, 8 pages.
A 3MPixel Multi-Aperture Image Sensor with 0.7μm Pixels in 0.11μm CMOS, Fife et al., Stanford University, 2008, 3 pages.
Dual camera intelligent sensor for high definition 360 degrees surveillance, Scotti et al., Publisher: IET, May 9, 2000, 8 pages.
Dual-sensor foveated imaging system, Hua et al., Publisher: Optical Society of America, Jan. 14, 2008, 11 pages.
Defocus Video Matting, McGuire et al., Publisher: ACM SIGGRAPH, Jul. 31, 2005, 11 pages.
Compact multi-aperture imaging with high angular resolution, Santacana et al., Publisher: Optical Society of America, 2015, 10 pages.
Multi-Aperture Photography, Green et al., Publisher: Mitsubishi Electric Research Laboratories, Inc., Jul. 2007, 10 pages.
Multispectral Bilateral Video Fusion, Bennett et al., Publisher: IEEE, May 2007, 10 pages.
Super-resolution imaging using a camera array, Santacana et al., Publisher: Optical Society of America, 2014, 6 pages.
Optical Splitting Trees for High-Precision Monocular Imaging, McGuire et al., Publisher: IEEE, 2007, 11 pages.
High Performance Imaging Using Large Camera Arrays, Wilburn et al., Publisher: Association for Computing Machinery, Inc., 2005, 12 pages.
Real-time Edge-Aware Image Processing with the Bilateral Grid, Chen et al., Publisher: ACM SIGGRAPH, 2007, 9 pages.
Superimposed multi-resolution imaging, Carles et al., Publisher: Optical Society of America, 2017, 13 pages.
Viewfinder Alignment, Adams et al., Publisher: Eurographics, 2008, 10 pages.
Dual-Camera System for Multi-Level Activity Recognition, Bodor et al., Publisher: IEEE, Oct. 2014, 6 pages.
Engineered to the task: Why camera-phone cameras are different, Giles Humpston, Publisher: Solid State Technology, Jun. 2009, 3 pages.
Related Publications (1)
Number Date Country
20240247953 A1 Jul 2024 US
Provisional Applications (1)
Number Date Country
63059200 Jul 2020 US
Continuations (1)
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Parent 17628905 US
Child 18591012 US