This application claims priority to Chinese patent applications CN 201820230284.7 and 201810132134.7, both filed on Feb. 9, 2018, and the entire contents of which are incorporated herein by reference.
The invention relates to a rotary apparatus having a rotary body, such as a body of a surgical microscope or a head of surgical microscope (including an ocular and a lens) connected to a linkage piece in a surgical microscope system, which can be pivoted or swiveled about at least one rotary shaft and which can maintain its position or posture after being pivoted or swiveled. For example, the body of a surgical microscope can be pivoted about a fifth axis and sixth axis of the surgical microscope system. More specifically, the invention relates to a self-balancing device for maintaining a position of the rotary body of the rotary apparatus during its rotation when changing the center of gravity of the rotary body relative to the rotary shaft.
An apparatus, which has a main working component being arranged to protrude from a frame or a base thereof and being able to pivot or swivel about one or more rotary shafts, is known. Here, the main working component is called “rotary body”, and thus the apparatus including such a working component is called “rotary apparatus,” wherein the rotary body needs to be held in a position after pivoting or swiveling when the center of gravity of the rotary body is changed relative to the rotary shaft to permit an operator to work with this rotary body. Such an apparatus is commonly found in the medical facility field, e.g., in the form of a surgical microscope apparatus or a dental diagnosis instrument. In order to allow a suspended rotary body to rotate easily, stop freely, and maintain any position after being pivoted or swiveled, it is known to provide a self-balancing device configured to withstand a new torque (hereafter referred to as “unbalancing torque”) generated by the rotary body relative to the rotary shaft due to the change in the center of gravity after pivoting or swiveling, thereby allowing the rotary body to be held in any desired position.
U.S. Pat. No. 5,492,296 discloses an adjustable stand for an optical viewing apparatus such as a surgical microscope. The adjustable stand includes a tilt shaft and a pivot shaft for the microscope. In order to keep the surgical microscope in balance, this patent proposes an energy store for balancing or counterbalancing the gravity torque (i.e., the unbalancing torque) of the surgical microscope, which is formed by a spiral flat spring mounted in a spring housing. The spring housing is located in the carrier connected to the tilt shaft and is rotatable relative thereto with the rotation of the tilt shaft. In this case, when the tilt shaft is rotated (i.e., when the position of the surgical microscope is changed), the spiral flat spring in the spring housing receives the torque developed by the rotation, thereby keeping the surgical microscope in balance even if the center of gravity of the surgical microscope is changed.
However, the above known technical solution suffers from multiple defects. First of all, the torque output from the spiral flat spring is linear, while the center of gravity of the surgical microscope body generally follows a sine curve or a cosine curve relative to the unbalancing torque caused by displacement of the rotary shaft. As a result, the known balancing system has certain limitations in terms of principle or effect and cannot produce a good balancing effect. Secondly, the spiral flat spring is susceptible to degradation of strength caused by repeated bending over a long period of time because of its inherent fatigue strength, and it may even run the risk of fatigue failure. Finally, in order to ensure strength, the balancing system of spiral flat spring type may need a greater mounting space.
The invention solves the problems in the above-described prior art and provides a novel balancing device. The balancing device outputs torsional torque by using permanent magnets facing to each other. This is a non-contact torque output technique and does not cause fatigue failure. Moreover, the torsional torque thereby generated is changed according to a sine or cosine curve, which matches well the unbalancing torque of a rotary body that needs to be compensated.
In the invention, the term “rotary body” refers to a working component which is extended/protruded or suspended relative to a frame or base of the apparatus, and which can pivot or swing around at least one rotary shaft and needs to be maintained in position after being pivoted or swiveled. Accordingly, the apparatus that includes the rotary body is called “rotary apparatus.”
Specifically, a balancing device for a rotary apparatus is provided, the rotary apparatus has a rotary body which is able to pivot or swivel about at least one rotary shaft. According to an aspect of the invention, the balancing device includes a magnet assembly and a torque adjusting mechanism, wherein the magnet assembly at least includes a combination of two or more magnets, and the torque adjusting mechanism is configured to adjust a torque generated by the combination of the two or more magnets.
The balancing device according to various aspects of the invention has the following advantageous technical features, which can be applied solely or in combination in any possible technical manners:
the torque is a torque for balancing/counteracting a torque generated by the center of gravity of the rotary body relative to the rotary shaft;
the two or more magnets include magnetizers;
the magnet assembly includes a first magnet and a second magnet movable relative to each other;
the torque adjusting mechanism is configured to adjust an electric current or a relative position of the two or more magnets so as to adjust the torque generated by the two or more magnets;
the magnets can be radial ring magnets or Halbach array magnets; Neodymium Iron Boron (NdFeB) magnets, samarium cobalt magnets, aluminum-nickel-cobalt magnets, ferrite magnets; permanent magnets, soft magnets, or electromagnets;
the torque adjusting mechanism includes a magnet phase adjusting mechanism, which is configured to adjust an initial relative phase of the poles of the first magnet and/or the second magnet;
the torque adjusting mechanism includes a torque amplitude adjusting mechanism, the torque amplitude adjusting mechanism is configured to adjust a coupling of the first magnet and/or the second magnet;
the balancing device includes a balancing device housing fixedly connected to a frame of the rotary apparatus;
the first magnet and/or the second magnet is/are connected to the rotary shaft in a non-rotatable manner;
the first magnet and the second magnet are each in an annular shape, wherein the second magnet has an inner diameter larger than an outer diameter of the first magnet, and is arranged substantially coaxial with the first magnet, wherein the first magnet and the second magnet are configured to be rotatable relative to each other;
the first magnet and/or the second magnet is/are formed by a plurality of magnet blocks arranged in Halbach array;
the torque amplitude adjusting mechanism includes a drive which is configured to translate at least one of the first and/or the second magnets relative to each other to permit the coupling of the two magnets to change gradually and/or in a stepped manner;
the coupling is defined as the area of a facing part between the first magnet and the second magnet;
the drive includes a first drive member which carries the first magnet or the second magnet and is arranged to translate along the rotary shaft, and a second drive member which can be operated outside of the balancing device housing to actuate the first drive member to translate;
the first drive member is formed by a sleeve slider mounted on the rotary shaft, the sleeve slider having an internal thread at a side facing the second drive member; the second drive member includes a sleeve portion and/or rod portion which have/has an external thread at a side facing the first drive member for engaging the internal thread;
the second drive member further includes a manipulation member connected to the sleeve portion and/or the rod portion and located outside of the balancing device housing, the manipulation member is used to manipulate the torque amplitude adjusting mechanism;
the manipulation member is configured to have a structure like a steering wheel or a rudder, or is in the form of a hand wheel;
the torque amplitude adjusting mechanism further includes a magnet position indicator which include a follow-up member associated with the first magnet or the second magnet, and a display unit visible from the outside of the balancing device, the follow-up member is configured to change a display state of the display unit as a function of a movement of the first magnet or the second magnet;
the follow-up member includes a push rod and a sleeve cone, an end of the push rod is placed on an outer surface of the sleeve cone that is translatable with the first magnet or the second magnet to permit to reciprocate in a radial direction along with axial translation of the first or second magnet; the display state of the display unit is set to change with the radial reciprocating movement of the push rod;
the magnet phase adjusting mechanism includes a member that can be operated from outside of the balancing device to impart rotation of the first magnet and/or the second magnet;
the magnet phase adjusting mechanism includes a rotating ring arranged on an outer peripheral surface of the balancing device housing;
the magnet phase adjusting mechanism further includes a locking ring, which is arranged side by side with the rotating ring on the outer peripheral surface of the balancing device housing and which has teeth on an end face opposite to the rotating ring configured for engaging with teeth on a corresponding end face of the rotating ring;
the magnet phase adjusting mechanism includes a worm gear configured to rotate with the first magnet or the second magnet, and a worm mounted in the balancing device housing and extending to the outside thereof for rotating the worm to cause the worm gear and the first magnet or the second magnet to rotate;
an end of the worm extending to the outside of the balancing device housing is provided with a hand wheel for manipulation;
the balancing device is arranged on a rotary shaft segment of the rotary shaft, is detachably connected to the rest of the rotary shaft;
the torque adjusting mechanism is driven by an electric motor; and
the rotary apparatus is a surgical microscope system, and the rotary body is a body of surgical microscope.
The invention will now be described with reference to the drawings wherein:
Referring to
In use, the body 1 of surgical microscope is aligned with a surgical site of the patient quickly and accurately. For this, the body 1 of surgical microscope is required to swivel from left to right or to pivot back and forth about the rotary shafts 5a and 6a, respectively, as a rotary body, and to maintain its position after it has been pivoted or swiveled over a certain angle. However, such movements will result in a change in the center of gravity of the body 1 of the surgical microscope relative to the position of the rotary shafts, and thus generate a new unbalancing torque relative to the corresponding rotary shaft. This unbalancing torque makes the body 1 of surgical microscope tend to move (pivot or swivel) after being aligned with the surgical site of the patient.
In addition, sometimes it is necessary to attach an assistant scope (co-observer) (not shown) to the body 1 of the surgical microscope to allow an auxiliary, e.g., an assistant of a doctor, to view the process of an operation. Usually, this assistant scope is relatively heavy and attached to extend a relative long distance from the body 1 of the surgical microscope. Consequently, the attachment of the assistant scope also results in a significant change in the center of gravity of the whole rotary body, and thus generates an unbalancing torque. Similarly, the unbalancing torque imparts a tendency of moving continuously to the rotary body including the body 1 of the surgical microscope and the assistant scope.
For counteracting or eliminating the above unbalancing torque so as to prevent the body 1 of the surgical microscope from moving forward and to allow the body 1 of the surgical microscope to rest and stop in an angular position after being pivoted or swiveled, a balancing device is provided for the body 1 of the surgical microscope according to an exemplary embodiment of the invention. In the following, the balancing device arranged on the rotary shaft 6a according to the exemplary embodiment is described. However, it should be understood that the balancing device may also be arranged on the rotary shaft 5a to keep the body 1 of the surgical microscope in balance relative to the rotary shaft 5a. It can be also be conceived to arrange the balancing device on both the rotary shaft 5a and the rotary shaft 6a.
The invention provides a magnetic balancing device including a magnet assembly and a torque adjusting mechanism. The magnet assembly includes at least two magnets movable, e.g. rotatable and translatable, relative to each other. The torque adjusting mechanism may include a mechanism for adjusting the coupling of the two magnets, and a mechanism for adjusting initial relative phases of the two magnets. The two magnets may consist of two spaced permanent magnets or electromagnets and may output a torsional torque which follows a cosine curve or a sine curve in a non-contact manner.
Referring to
In this way, when an operator, such as a surgeon, pulls, pushes, rotates or swivels the body 1 of the surgical microscope mounted on the rotary shaft 6a to adjust its position or posture, the rotary shaft 6a rotates with the rotation of the body 1 of the surgical microscope, and meanwhile the first magnet 11 rotates with the rotation of the rotary shaft 6a. At this time, the second magnet 12 arranged in the balancing device housing 13 is kept stationary. The relative rotation between the first magnet 11 and the second magnet 12 generates a torsional torque which follows a cosine curve or a sine curve by a magnetic force, such that the unbalancing torque generated by the rotation of the body 1 of the surgical microscope relative to the rotary shaft 6a may be counteracted.
According to a first exemplary embodiment of the invention, as shown in
In this case, typically, the outer magnet 12 is formed by a plurality of, typically twelve magnet blocks which are bonded to form a ring and in a Halbach array in terms of magnetizing direction and positions, as shown in
Still referring to
The torque amplitude adjusting mechanism may be configured in such a manner that the first magnet 11 as the inner magnet and the second magnet 12 as the outer magnet are relatively moved gradually among a fully coupled state (as shown in
Specifically, when the first magnet 11 and the second magnet 12 are fully coupled, i.e., when the first magnet 11 is placed entirely inside the second magnet 12, the area of the facing part between the outer surface of the first magnet 11 and the inner surface of the second magnet 12 is maximal, and a maximum amplitude of torsional torque generated by the relative rotation of 360° is created. When the first magnet 11 and the second magnet 12 are partly coupled, i.e., when the first magnet 11 is placed partly inside the second magnet 12, an intermediate amplitude of torsional torque generated during the relative rotation of 360° is created. When the first magnet 11 is separated from the second magnet 12, i.e., when there is no facing part between the outer surface of the first magnet 11 and the inner surface of the second magnet 12, the amplitude of torsional torque generated during the relative rotation of 360° is at a minimum or zero.
Returning to
As can be seen from
Still referring to
According to the first exemplary embodiment of the invention, the first drive member 21 in the form of a sleeve slider has an internal thread at a side away from the rotary shaft 6a, the internal thread extending over a certain length in an axial direction of the first drive member 21 (i.e., in a left-right direction in
In this way, when the second drive member 22 is rotated, due to thread screwing of its external thread with the internal thread of the first drive member 21, the first drive member 21 carrying the first magnet 11 will translate or slide along the axial direction on the rotary shaft segment 16, thus changing the area of the facing part between the first magnet 11 and the second magnet 12. In this process, there is no relative rotation among the first magnet 11, the first drive member 21, and the rotary shaft 6a. The rotary shaft 6a and the rotary shaft segment 16 are also configured to not rotate with the rotation of the second drive member 22.
As an alternative exemplary embodiment not shown in the drawings, it is possible that the first drive member 21 and the second drive member 22 are combined to form a single drive member. The single drive member is configured as, e.g., a sleeve mounted on the rotary shaft segment 16 and having an internal thread. The internal thread of the sleeve engages the external thread on the corresponding rotary shaft segment 16 so as to translate the first magnet 11 on the rotary shaft segment 16 by gradually screwing in and out.
Back to
It should be understood that although in the above described first exemplary embodiment, the first magnet 11 is arranged to move in the axial direction of the rotary shaft to change facing areas of the first magnet 11 and the second magnet 12, it is also possible to make the first magnet 11 stationary while the second magnet 12 is movable, or to make both the first and the second magnets 11 and 12 movable, so as to change the range of facing areas between the two magnets, that is to change the coupling state thereof.
Still as shown in
In this way, the magnet shell 14 may be driven by rotating the rotating ring 31 outside of the balancing device 100, and thereby causing the second magnet 12 to rotate, which changes the relative phase between the second magnet 12 and the first magnet 11.
Typically, the magnet phase adjusting mechanism 30 further includes a locking ring 32 arranged side by side with the rotating ring 31 on the outer peripheral surface of the balancing device housing 13. In particular, the locking ring 32 is provided with teeth on an axial end face opposing to the rotating ring 31 so as to engage with teeth arranged correspondingly on the rotating ring 31, thereby locking the rotating ring 31 upon completion of the phase adjustment.
The magnet phase adjusting mechanism 30 is not limited to the above exemplary embodiments, and the adjustment of initial phase may be achieved either by rotating the first magnet 11 or by rotating the second magnet 12. For example, it can be conceived to form raised portions (not shown) on the magnet shell 14 which accommodates the second magnet 12, and the raised portions are configured to be exposed or accessed through sliding slots formed in the balancing device housing 13 from the outside of the balancing device 100, such that it is possible to rotate the magnet housing 14 and the second magnet 12 contained therein. For example, teeth (not shown) may be disposed on the flange 210 of the first drive member 21 and may be used to control and adjust the rotation of the first magnet 11, so as to realize the adjustment of relative phase. Here, accordingly, the torque amplitude adjusting mechanism is configured to cause the second magnet 12 to move relative to the first magnet 11.
When a surgical microscope apparatus shown in
The initial relative phase of the first magnet 11 and the second magnet 12 are adjusted by the magnet phase adjusting mechanism 30, depending on the center of gravity of the body 1 of the surgical microscope relative to the rotary shaft 6a. That is, the initial relative angle between a connection line of the N and S poles of the first magnet 11 and a connection line of the N and the S poles of the second magnet 12 is adjusted. Specifically, referring to
The initial setting may be carried out in another way according to an exemplary embodiment: when the magnets are decoupled, that is, when the facing area of the first magnet 11 and the second magnet 12 is minimal or when the first magnet 11 is farthest from the second magnet 12, the rotary body moves freely, and the center of gravity of the rotary body is just vertically below the rotary shaft 6a after moving, the relative phase of the first magnet 11 and the second magnet 12 is directly adjusted to be zero (i.e., the S pole of the first magnet 11 and the N pole of the second magnet 12 is aligned with each other). Next, the coupling between the first magnet 11 and the second magnet 12 is increased by the torque amplitude adjusting mechanism. Finally, the rotary body is centralized to be ready for use under a certain appropriate coupling, thus, the torque output by the magnet assembly and the unbalancing torque generated by the rotary body are matched.
After the above setting and adjustment, the surgical microscope system is ready for use, and the body 1 of the surgical microscope may be pivoted or swiveled to any position relative to the rotary shaft 6a as needed by the operator during its use. Thanks to the balancing device 100 of the invention, the body 1 of the surgical microscope always maintains its angular position without continuous pivoting or swiveling if it is released by the operator after being rotated a certain angle about the rotary shaft 6a. This is due to the fact that the balancing device 100 outputs a torsional torque following a cosine (or sine) curve (as shown in
Another exemplary embodiment of the invention is illustrated below with reference to
The main difference between the balancing device illustrated in the exemplary embodiment shown in
Referring to
As shown in
The follow-up member may be configured to move with the movement of the first magnet 11 so as to indicate a display mark of the display unit 236.
Returning to
Now referring to
The balancing device of this exemplary embodiment can be used in the following manner. If the surgical microscope apparatus is only equipped with the body 1 of the surgical microscope, the operator may place the first magnet and the second magnet in the coupling state of “without co-observer” by the torque amplitude adjusting mechanism and with reference to the display marks displayed by the display unit 236, and adjust the initial phase of the first magnet and the second magnet by the magnet phase adjusting mechanism 30′, so as to achieve the balance of the rotary body which only includes the body 1 of the surgical microscope. If the assistant scope is attached to the body 1 of the surgical microscope, the operator may place the first magnet and the second magnet in the coupling state of “with co-observer” by the torque amplitude adjusting mechanism, and adjust the initial phase of the first magnet and the second magnet by the magnet phase adjusting mechanism 30′, so as to achieve the balance of the rotary body including the body of surgical microscope and the assistant scope. Of course, the exemplary embodiment may be modified to apply for a rotary apparatus having more than two significant different weights, as long as the corresponding display marks of the display unit 236 are modified accordingly. For example, when an external camera or any other structure is attached to the body of surgical microscope, an additional display mark can be added to the display unit 236.
According to another exemplary embodiment which is not shown, operation(s) of the torque amplitude adjusting mechanism and/or the magnet phase adjusting mechanism may be realized by a drive of an electric motor. The adjustment may be automatic torsional torque detection and automatic torque generation adjustments by sensors and electrical means.
Although the exemplary embodiments illustrated hereinabove include a surgical microscope system, it should be understood that the application field of the invention is not limited thereto. Instead, the present invention may be applied to any rotary apparatus with a rotary body, for example, processing or operating equipment in the industrial field, tower crane equipment in the construction field, etc. The first and second magnets used in the exemplary embodiments of the invention may be of various types of magnets, such as radial ring magnets or Halbach array magnets, for example, NdFeB magnets, samarium cobalt magnets, aluminum-nickel-cobalt magnets or ferrite magnets, such as permanent magnets or soft magnets or electromagnets.
Finally, it is understood that the foregoing description is that of the exemplary embodiments of the invention and that various changes and modifications may be made thereto without departing from the spirit and scope of the invention as defined in the appended claims.
Number | Date | Country | Kind |
---|---|---|---|
201810132134.7 | Feb 2018 | CN | national |
201820230284.7 | Feb 2018 | CN | national |
Number | Name | Date | Kind |
---|---|---|---|
2771171 | Schultz | Nov 1956 | A |
2807734 | Lehde | Sep 1957 | A |
3050646 | Eddy | Aug 1962 | A |
3394295 | Cory | Jul 1968 | A |
3407318 | Korthaus | Oct 1968 | A |
3555321 | Gruener | Jan 1971 | A |
3822390 | Janson | Jul 1974 | A |
3934216 | Ward | Jan 1976 | A |
4115040 | Knorr | Sep 1978 | A |
4152617 | Janson | May 1979 | A |
4163164 | Pieters | Jul 1979 | A |
4239092 | Janson | Dec 1980 | A |
4371798 | Kuroda | Feb 1983 | A |
4381466 | Laenens | Apr 1983 | A |
4943019 | Mester | Jul 1990 | A |
5064029 | Araki | Nov 1991 | A |
5096024 | Wu | Mar 1992 | A |
5158279 | Laffey | Oct 1992 | A |
5204572 | Ferreira | Apr 1993 | A |
5248940 | Patience | Sep 1993 | A |
5254061 | Leask | Oct 1993 | A |
5288043 | Tigliev | Feb 1994 | A |
5437353 | Wu | Aug 1995 | A |
5455473 | Lipo | Oct 1995 | A |
5468201 | Minoura | Nov 1995 | A |
5480114 | Nakamura | Jan 1996 | A |
5492296 | Biber | Feb 1996 | A |
5528417 | Nakamura | Jun 1996 | A |
5583408 | Lowrance | Dec 1996 | A |
5675203 | Schulze | Oct 1997 | A |
5779456 | Bowes | Jul 1998 | A |
5783885 | Post | Jul 1998 | A |
5793826 | Sato | Aug 1998 | A |
5831364 | Buse | Nov 1998 | A |
5880548 | Lamb | Mar 1999 | A |
6041571 | Fields | Mar 2000 | A |
6099467 | Kehr | Aug 2000 | A |
6129194 | Booth | Oct 2000 | A |
6186023 | Nakamura | Feb 2001 | B1 |
6218751 | Bohlin | Apr 2001 | B1 |
6234938 | Chen | May 2001 | B1 |
6429611 | Li | Aug 2002 | B1 |
6555941 | Zepp | Apr 2003 | B1 |
6682430 | Killen | Jan 2004 | B2 |
6737778 | Daikoku | May 2004 | B2 |
6841909 | Six | Jan 2005 | B2 |
6943478 | Zepp | Sep 2005 | B2 |
7034427 | Hirzel | Apr 2006 | B2 |
7219864 | Strauss | May 2007 | B2 |
7294947 | Corbin, III | Nov 2007 | B2 |
7598646 | Cleveland | Oct 2009 | B2 |
7741746 | Groening | Jun 2010 | B2 |
7863789 | Zepp | Jan 2011 | B2 |
7960888 | Ai | Jun 2011 | B2 |
8221247 | Lai | Jul 2012 | B2 |
8240447 | Ueda | Aug 2012 | B2 |
8904900 | Dorigatti | Dec 2014 | B2 |
8910537 | Nakamura | Dec 2014 | B2 |
9103150 | Wong | Aug 2015 | B1 |
9638273 | Schmidt | May 2017 | B2 |
9748886 | McDonald | Aug 2017 | B1 |
9855069 | Jezierski | Jan 2018 | B2 |
10016900 | Meyer | Jul 2018 | B1 |
10374502 | Diao | Aug 2019 | B2 |
10589935 | Ragan | Mar 2020 | B2 |
20020093262 | Zepp | Jul 2002 | A1 |
20020186647 | Her | Dec 2002 | A1 |
20040066107 | Gery | Apr 2004 | A1 |
20040130228 | Chang | Jul 2004 | A1 |
20050104469 | Zepp | May 2005 | A1 |
20060261765 | Prasanna | Nov 2006 | A1 |
20070000741 | Pribonic | Jan 2007 | A1 |
20080054748 | Huber | Mar 2008 | A1 |
20080105078 | Gregor | May 2008 | A1 |
20080105503 | Pribonic | May 2008 | A1 |
20080150383 | Groening | Jun 2008 | A1 |
20090004037 | Ito | Jan 2009 | A1 |
20090125024 | Baur | May 2009 | A1 |
20090163929 | Yeung | Jun 2009 | A1 |
20100138127 | Boughtwood | Jun 2010 | A1 |
20100156227 | Hung | Jun 2010 | A1 |
20100163694 | Fadler | Jul 2010 | A1 |
20100308149 | Allington | Dec 2010 | A1 |
20110037333 | Atallah | Feb 2011 | A1 |
20110045932 | Fauteux | Feb 2011 | A1 |
20110057530 | Chang | Mar 2011 | A1 |
20110162476 | Nakamura | Jul 2011 | A1 |
20120262017 | Mengibar Rivas | Oct 2012 | A1 |
20120296159 | Kanazawa | Nov 2012 | A1 |
20130123026 | Purdy | May 2013 | A1 |
20130205558 | Sporer | Aug 2013 | A1 |
20130285482 | Yamamoto | Oct 2013 | A1 |
20130299299 | Hoffmann | Nov 2013 | A1 |
20140157937 | Doi | Jun 2014 | A1 |
20140167545 | Bremner | Jun 2014 | A1 |
20150042182 | Glover | Feb 2015 | A1 |
20150171694 | Walsh | Jun 2015 | A1 |
20150200582 | Headstrom | Jul 2015 | A1 |
20150250547 | Fukushima | Sep 2015 | A1 |
20150301553 | Rossa | Oct 2015 | A1 |
20150369418 | Wong | Dec 2015 | A1 |
20160036308 | Bailey | Feb 2016 | A1 |
20160223031 | Atkinson | Aug 2016 | A1 |
20160242728 | Niizeki | Aug 2016 | A1 |
20160329795 | Ricci | Nov 2016 | A1 |
20160367334 | Devengenzo | Dec 2016 | A1 |
20170027652 | Johnson | Feb 2017 | A1 |
20170317573 | Mueller | Nov 2017 | A1 |
20170353078 | Post | Dec 2017 | A1 |
20180014906 | Fukushima | Jan 2018 | A1 |
20180110581 | Kamata | Apr 2018 | A1 |
20180212500 | Bendixen | Jul 2018 | A1 |
20180219452 | Boisclair | Aug 2018 | A1 |
20180264655 | Kuroda | Sep 2018 | A1 |
20180358870 | Kawanami | Dec 2018 | A1 |
20190046283 | Nagao | Feb 2019 | A1 |
20190109549 | Odagiri | Apr 2019 | A1 |
20190312497 | Walsh | Oct 2019 | A1 |
20190328480 | Kamikawa | Oct 2019 | A1 |
20200129052 | Unai | Apr 2020 | A1 |
20200266682 | Goossens | Aug 2020 | A1 |
20200343805 | Rhyu | Oct 2020 | A1 |
20200386289 | Clymer | Dec 2020 | A1 |
Number | Date | Country |
---|---|---|
WO-2017015764 | Feb 2017 | WO |
Number | Date | Country | |
---|---|---|---|
20190250360 A1 | Aug 2019 | US |