DC-DC converter switching transistor current measurement technique

Information

  • Patent Grant
  • 9124174
  • Patent Number
    9,124,174
  • Date Filed
    Monday, June 10, 2013
    11 years ago
  • Date Issued
    Tuesday, September 1, 2015
    8 years ago
Abstract
A method is described comprising conducting a first current through a switching transistor. The method also comprises conducting a second current through a pair of transistors whose conductive channels are coupled in series with respect to each other and are together coupled in parallel across the switching transistor's conductive channel. The second current is less than and proportional to the first current.
Description
BACKGROUND

DC-DC converters typically craft a DC voltage by full wave rectifying and filtering one or more time varying signals. Because of the switching undertaken in the full wave rectification process, significant amounts of current are frequently “switched” back-and-forth at rapid pace by large transistors. It is often helpful to measure the current through these transistors to, for instance, determine whether or not the DC-DC converter is being loaded, monitor any ripple currents resulting from rectification, etc.


Two “straight-forward” techniques are readily known in the art for measuring current: 1) shunt inductance; and, 2) series resistance. Shunt inductance induces a current measurement signal in an inductor by coupling magnetic fields that are produced by the current signal being measured through the inductor. Unfortunately, shunt inductance is not practical for rapidly changing currents because the bandwidth of an inductor is limited (i.e., the inductor will increasingly attenuate the current measurement signal as its frequency increases).


The series resistance technique, which is shown in FIG. 1, does not typically suffer from limited bandwidth issues because a pure resistance does not change its resistive properties as a function of signal frequency. Unfortunately, however, the series resistance technique is also not practical for large currents (such as those drawn by a DC-DC converter's switching transistors) because a large current being driven through a resistance will tend to dissipate large amounts of power (through the relationship P=I2R) which may result in overheating; or, if the power “problem” is handled by using a very small series resistance, inaccuracy results because the signal V=I*R may become too small to measure.





FIGURES

The present invention is illustrated by way of example and not limitation in the figures of the accompanying drawings, in which like references indicate similar elements and in which:



FIG. 1 shows resistance couples in series with a DC-DC converter switching transistor;



FIG. 2 shows an embodiment of a current measurement circuit coupled to a DC-DC converter switching transistor;



FIG. 3 shows an equivalent circuit for the circuit of FIG. 2;



FIG. 4 shows another circuit that measures DC-DC converter switching transistor current using a similar M1 through M4 structure as shown in FIG. 2;



FIG. 5 shows an extension of the circuit of FIG. 4 capable of providing an indication of the output current from the pair of switching transistors Q1 and Q2;



FIG. 6 shows a computing system whose processor(s) include a DC-DC converter.





DETAILED DESCRIPTION


FIG. 2 shows a circuit directed to measuring the IDS current of transistor Q1 without the use of a series resistance through which the IDS current flows. Here, transistor Q1 may be a large switching transistor whose drain-to-source current (IDS) is rapidly changing with large amplitude. A pair of transistors M1, M2 having their conductive channels coupled in series (where, the conductive channel of a transistor is understood to be the channel between its drain and source nodes). The drain of M1 is coupled to the drain of the switching transistor's conductive channel. The source of M2 is coupled to the source of the switching transistor's conductive channel (through the ground node). A node between the M1 and M2 transistors is coupled to an input of an amplifier (the source node of M5). A second pair of transistors M3 and M4 have their conductive channels coupled in parallel (their drains are tied together and their source nodes are tied to ground) and a node between the second pair of transistors M3, M4 is coupled to a reference input of the amplifier (the source node of M6).


According to the theory of operation of the circuitry of FIG. 2, a current flow of approximately kIDS will flow through transistor M1, where k<1 (e.g., in many applications k is expected to be within a range of 0.0001 to 0.01 inclusive). The kIDS current flow through transistor M1 influences an output signal Io which can be used as an indicator of the current IDS through transistor Q1. In a typical implementation transistors M1 and M2, as well as M3 and M4 are scaled down versions of transistor Q1 (e.g., being designed with identical doping profiles and gate lengths but with different gate widths). Since a large transistor Q1 is often implemented as a parallel connection of many identical small transistors (legs), the smaller transistors M1, M2, M3, and M4 can be implemented using just a few of the same small transistors.


The proportionality factor can be approximately computed from the transistors' widths as 1/k=WQ1*(1/WM1+1/WM2). In some applications a value of k>1 may be desirable. The M1 and M2 structure essentially enables fast and accurate measurement of the IDS current without actually imposing a series resistance through the IDS current path. To ensure proper operation, M1 and M3 may be matched and M2 and M4 may be matched respectively. To improve the accuracy at larger drain-to-source voltages VDS in Q1, especially, when Q1 is operating in saturation, M1 may be chosen to be smaller than M2. To enhance the output signal Io, M1 may be chosen to be larger than M2.


Transistors M5, M6, M7 and M8 form a common gate amplifier having: 1) a reference leg M6, M7 whose current, TBIAS, flows into the resistive network formed by transistors M3 and M4; and, 2) a measurement leg M5, M8 whose current Ix flows into the resistive network formed by transistors M1 and M2.


The principle of operation of the entire circuit is that voltage changes in proportion to kIDS at the source of transistor M5 causes the gate-to-source voltage of transistor M5 to differ with respect to that of transistor M6 such that an output current Io is created having a component that varies in proportion to kIDS. The current IBIAS may be injected using various techniques, such as, e.g., using a reference current circuit or a resistor connected to the gates of M6 and M7.


The principle of operation of the circuit of FIG. 2 is more easily viewed with the equivalent circuit of FIG. 3. Comparing FIGS. 2 and 3, note that: 1) transistor M1 has been replaced by a variable resistance R1 and a voltage source VDS causing a current of kIDS; 2) transistor M2 has been replaced by resistance R2; 3) transistor M3 has been replaced by variable resistance R3; and, 4) transistor M4 has been replaced by resistance R4.


Transistors M2 and M4 are designed to be in the linear mode over the range of operation for the circuit. Therefore, M2 and M4 will behave like resistors (i.e., approximately a linear relationship between its drain-to-source voltage and its drain-to-source current). Moreover, like M2 and M4, transistors M1 and M3 are also ideally designed to remain in linear mode of operation, when transistor Q1 is in linear mode, and to be in saturation mode when Q1 is in saturation mode. In order to help effect this behavior, the gates of transistors M2 and M4 are tied to a fixed voltage (VCC) and the gates of transistors M1 and M3 are tied to the gate of transistor Q1.


With transistors M5 and M6 in saturation mode, and with transistors M7 and M8 forming a current mirror, it can be shown that the output current Io for the circuit of FIG. 3 can be approximated as:

Io≈kIDS(R1/(R1//R2+R5))+((R1//R1//R2)−(R3//R4))/R1//R2+R5))IBIAS  Eqn. 1

where IDS is the current being measured (i.e., the drain-to-source current of transistor Q1), k is a proportionality constant between the drain-to-source currents of transistors Q1 and M1, and R5 is the common-gate input resistance of transistor M5. Moreover,

R3//R4=(R3R4)/(R3+R4)  Eqn. 2a
R1//R2=(R1R2)/(R1+R2)  Eqn. 2b

which corresponds to the effective resistances of resistors R3 and R4 in parallel and R1 and R2 in parallel, respectively. Since R1=R3 and R2=R4, IBIAS does not add to the output signal Io. The value of R5 depends on the transconductance parameter β of M5 and on the bias current IBIAS:

R5=1/sqrt(2βM5(IBIAS−Io))  Eqn. 3

In a typical design R5 may be large compared to R1//R2, e.g., ten times larger, to reduce the power consumption of the common-gate amplifier. In other designs R5 may be comparable to or even smaller than R1//R2 in order to improve linearity. To ensure proper operation the bias current should be larger than the maximum output current: IBIAS>Io. For negative currents Io<0 the bias current may be reduced to a very small value, e.g., by operating M5 and M6 at or slightly above threshold. The presence of M3 also provides for good suppression of noise from the gate node of transistor Q1 since the noise injected through the gate capacitances of M1 and M3 approximately cancels out. Note that although the reference voltage of FIGS. 2 and 3 correspond to a ground node, another fixed voltage could be used (such as a supply node) provided appropriate offset were applied to VCC.


Other Circuits


FIG. 4 provides another circuit design that uses the M1 through M4 structure as a device for measuring IDS, but uses a different common-gate amplifier, formed by M5 through M11, to generate the output signal Io. This amplifier is essentially equivalent to a combination of two replicas of the amplifier M5 through M8 in FIG. 2 and provides improved range and linearity at a reduced bias current.


When the current IDS of Q1 is small, i.e., the output signal is approximately −IBIAS<Io<+IBIAS, both parts of the amplifier, M5 through M8 and M9 through M11 respectively. contribute to the output signal Io. When current is large and positive, i.e., Io>+IBIAS, M9 through M11 will increase their contribution to Io due to the nonlinearity of the circuit, whereas M5 through M8 will reduce and eventually cease their contribution to the output signal.


Furthermore, when the current is large and negative, i.e., Io<−IBIAS, M9 through M11 will reduce their contribution to Io and M5 through M8 will take over. Thus, the non-linearities of both halves of the amplifier compensate each other, resulting in improved linearity and range at a smaller bias current. The method for properly choosing the bias current IBIAS and the sizes of M5 through M11 usually involves simple calculations and circuit simulations, which anyone skilled in the art can easily carry out.



FIG. 5 shows a circuit that measures the current through both of switching transistors Q1 and Q2. M13 through M16 are the PMOS equivalent of M1 through M4 respectively, and, M7, M8, M11, M12 are coupled so that they become the PMOS equivalent of M5, M6, M10 and M9 respectively. Arrangement in this manner allows for an output Io that varies with IDSQ2−IDSQ1.


Possible Applications of Current Measurement Circuits

It is envisioned that embodiments of the current measurement approaches described herein can be used in “on-chip” DC-DC converters. A DC-DC converter is a device that converts a first fixed voltage into a second fixed voltage. Here, for example, transistor Q1 (and transistors Q1 and Q2 in FIG. 4) can be a large switching transistor in an “on-chip” DC-DC converter (and transistors Q1 and Q2 can be large switching transistors in an “on-chip” DC-DC converter).


The current measurement circuit can be used for various functions such as, to name a few: 1) soft-switching, i.e., to monitor the currents through switching transistors in order to determine the proper time for turn-off; 2) monitoring the ripple current in DC-DC converters; 3) “safe turn off” in “on-chip” DC-DC converters (e.g., turning off the DC-DC converter when the inductor currents flowing through the switching transistors are small enough to prevent voltage overshoot); and, 4) monitoring the load current, e.g., in “on-chip” DC-DC converters used to a CPU (central processing unit) or part of a CPU.



FIG. 6 shows an embodiment of a computing system. The exemplary computing system of FIG. 6 includes: 1) one or more processors 601 having an “on-chip” DC-DC converter 610; 2) a memory control hub (MCH) 602; 3) a system memory 603 (of which different types exist such as DDR RAM, EDO RAM, etc,); 4) a cache 604; 5) an I/O control hub (ICH) 605; 6) a graphics processor 606; 6) a display/screen 607 (of which different types exist such as Cathode Ray Tube (CRT), Thin Film Transistor (TFT), Liquid Crystal Display (LCD), DPL, etc.; 8) one or more I/O devices 608.


The one or more processors 601 execute instructions in order to perform whatever software routines the computing system implements. The instructions frequently involve some sort of operation performed upon data. Both data and instructions are stored in system memory 603 and cache 604. Cache 604 is typically designed to have shorter latency times than system memory 603. For example, cache 604 might be integrated onto the same silicon chip(s) as the processor(s) and/or constructed with faster SRAM cells whilst system memory 603 might be constructed with slower DRAM cells.


By tending to store more frequently used instructions and data in the cache 604 as opposed to the system memory 603, the overall performance efficiency of the computing system improves. System memory 603 is deliberately made available to other components within the computing system. For example, the data received from various interfaces to the computing system (e.g., keyboard and mouse, printer port, LAN port, modem port, etc.) or retrieved from an internal storage element of the computing system (e.g., hard disk drive) are often temporarily queued into system memory 603 prior to their being operated upon by the one or more processor(s) 601 in the implementation of a software program.


Similarly, data that a software program determines should be sent from the computing system to an outside entity through one of the computing system interfaces, or stored into an internal storage element, is often temporarily queued in system memory 603 prior to its being transmitted or stored. The ICH 605 is responsible for ensuring that such data is properly passed between the system memory 603 and its appropriate corresponding computing system interface (and internal storage device if the computing system is so designed). The MCH 602 is responsible for managing the various contending requests for system memory 603 access amongst the processor(s) 601, interfaces and internal storage elements that may proximately arise in time with respect to one another.


One or more I/O devices 608 are also implemented in a typical computing system. I/O devices generally are responsible for transferring data to and/or from the computing system (e.g., a networking adapter); or, for large scale non-volatile storage within the computing system (e.g., hard disk drive). ICH 605 has bi-directional point-to-point links between itself and the observed I/O devices 608.


In the foregoing specification, the invention has been described with reference to specific exemplary embodiments thereof. It will, however, be evident that various modifications and changes may be made thereto without departing from the broader spirit and scope of the invention as set forth in the appended claims. The specification and drawings are, accordingly, to be regarded in an illustrative rather than a restrictive sense.

Claims
  • 1. An apparatus, comprising: a direct-current to direct-current (DC-to-DC) converter circuit including a current measurement circuit having a first pair of transistors with respective channels of the first pair of transistors coupled in series, a drain of a first transistor of the first pair of transistors coupled to a first end of a conductive channel of a switching transistor, and a source of a second transistor of the first pair of transistors coupled to a second end of the channel of the switching transistor;an amplifier having a measurement leg coupled to a node between the first pair of transistors; anda second pair of transistors with respective channels of the second pair of transistor being coupled in parallel, a node between the second pair of transistors being coupled to a reference leg of the amplifier.
  • 2. The apparatus of claim 1, further comprising one or more processors coupled to an output of the measurement leg of the amplifier to monitor current of the DC-to-DC converter circuit.
  • 3. The apparatus of claim 2, wherein the one or more processors and the direct-current to direct-current converter circuit are formed on a single integrated circuit chip.
  • 4. The apparatus of claim 1, wherein a first of the second pair of transistors has a gate coupled to both a gate of the first transistor of the first pair of transistors and a gate of the switching transistor.
  • 5. The apparatus of claim 1, wherein a source of each of the second pair of transistors is tied to the switching transistor through a ground connection and the drains of each of the second pair of transistors are tied together.
  • 6. The apparatus of claim 1, wherein the first pair of transistors and the second pair of transistors have similar doping profiles and gate lengths as the switching transistor.
  • 7. The apparatus of claim 1, wherein the first pair of transistors and the second pair of transistors have different gate widths than the switching transistor.
  • 8. The apparatus of claim 1, wherein the switching transistor is comprised of a parallel coupling of a plurality of similar small transistors.
  • 9. The apparatus of claim 8, wherein the first pair of transistors and the second pair of transistors are implemented using four of the plurality of small transistors.
  • 10. The apparatus of claim 1, wherein the first transistor of the first pair of transistors and a first transistor of the second pair of transistors each impose substantially the same resistance in the DC-to-DC converter circuit, the resistance being greater than a resistance imposed by a second transistor of the second pair of transistors.
  • 11. A method, comprising: conducting a first current through a switching transistor of a direct-current to direct-current (DC-to-DC) converter circuit; andconducting a second current through a pair of transistors that are coupled to the switching transistor, the second current being less than and proportional to the first current, a common node of the pair of transistors being coupled to a measurement leg of an amplifier to produce an output signal for monitoring the first current.
  • 12. The method of claim 11, further comprising selecting a proportionality constant between the second current through the pair of transistors and the first current through the switching transistor to be less than 1.
  • 13. The method of claim 12, wherein the proportionality constant is selected to be within a range from about 0.0001 to about 0.01.
  • 14. The method of claim 11, further comprising using one or more processors coupled to the measurement leg of the amplifier to monitor the first current through the switching transistor.
  • 15. The method of claim 11, further comprising coupling a common node of a second pair of transistors to a reference input leg of the amplifier, the second pair of transistors being coupled to the source of the switching transistor.
  • 16. The method of claim 11, wherein the pair of transistors has serially-coupled conductive channels, the pair of transistors passing the second current through the conductive channels, the pair of transistors being coupled in parallel across a conductive channel of the switching transistor.
  • 17. The method of claim 11, wherein the first current is monitored without the use of a series resistance coupled in series with the switching transistor.
  • 18. The method of claim 11, wherein the proportional second current through the first transistor of the pair of transistors affects an output signal on the measurement leg of the amplifier in proportion to the current through the switching transistor.
  • 19. An apparatus to monitor current, the apparatus comprising: a direct-current to direct-current (DC-to-DC) converter circuit including one or more processors to monitor a current of the direct-current to direct-current converter circuit;a current measurement circuit having a pair of transistors with respective channels of the pair of transistors coupled in series, a drain of a first transistor of the pair of transistors coupled to a first end of a conductive channel of a switching transistor, and a source of a second transistor of the pair of transistors coupled to a second end of a channel of the switching transistor; andan amplifier having a measurement leg coupled to a node between the pair of transistors to receive a current from the pair of transistors that is smaller than and proportional to a drain-to-source current flowing through the switching transistor.
  • 20. The apparatus of claim 19, further comprising a second pair of transistors having their respective conductive channels coupled in parallel, a source of each of the second pair of transistors being tied to the switching transistor through a ground connection, a node between the second pair of transistors being coupled to a reference leg of the amplifier.
PRIORITY APPLICATION

This application is a continuation of U.S. application Ser. No. 13/417,763, filed Mar. 12, 2012, now issued as U.S. Pat. No. 8,482,552, and entitled “DC-DC Converter Switching Transistor Current Measurement Technique,” which is a divisional application of U.S. patent application Ser. No. 11/173,760, filed Jun. 30, 2005, now issued as U.S. Pat. No. 8,134,548, all of which are incorporated herein by reference in their entirety.

US Referenced Citations (82)
Number Name Date Kind
3607462 Laing Sep 1971 A
3881244 Kendall May 1975 A
3905883 Hanazono et al. Sep 1975 A
4055774 Ahmed Oct 1977 A
4543553 Mandai et al. Sep 1985 A
4791719 Kobayashi et al. Dec 1988 A
4797648 Kaneko et al. Jan 1989 A
4816784 Rabjohn Mar 1989 A
4884156 Miyakawa et al. Nov 1989 A
4959631 Hasegawa et al. Sep 1990 A
5047296 Miltenberger et al. Sep 1991 A
5053697 Carnel et al. Oct 1991 A
5095357 Andoh et al. Mar 1992 A
5121852 Wilkes Jun 1992 A
5169713 Kumurdjian Dec 1992 A
5221459 Okano et al. Jun 1993 A
5298857 Voisine et al. Mar 1994 A
5420558 Ito et al. May 1995 A
5446311 Ewen et al. Aug 1995 A
5469399 Sato et al. Nov 1995 A
5530415 Takaya et al. Jun 1996 A
5583474 Mizoguchi et al. Dec 1996 A
5609946 Korman et al. Mar 1997 A
5635892 Ashby et al. Jun 1997 A
5694030 Sato et al. Dec 1997 A
5696441 Mak et al. Dec 1997 A
5705287 Doerner et al. Jan 1998 A
5706189 Majumdar et al. Jan 1998 A
5781071 Kusunoki Jul 1998 A
5801100 Lee et al. Sep 1998 A
5834825 Imai Nov 1998 A
5877533 Arai et al. Mar 1999 A
5892425 Kuhn et al. Apr 1999 A
5920979 Nepela et al. Jul 1999 A
5930415 Pham Jul 1999 A
5952704 Yu et al. Sep 1999 A
5961746 Nepela Oct 1999 A
5976715 Chen et al. Nov 1999 A
6031445 Marty et al. Feb 2000 A
6033782 Hubbard et al. Mar 2000 A
6037649 Liou Mar 2000 A
6040226 Wojnarowski et al. Mar 2000 A
6043641 Singer et al. Mar 2000 A
6067002 Fujino et al. May 2000 A
6103136 Han et al. Aug 2000 A
6114937 Burghartz et al. Sep 2000 A
6121852 Mizoguchi et al. Sep 2000 A
6166422 Qian et al. Dec 2000 A
6191495 Kossives et al. Feb 2001 B1
6194987 Zhou et al. Feb 2001 B1
6201287 Forbes Mar 2001 B1
6207303 Tomita Mar 2001 B1
6240621 Nellissen et al. Jun 2001 B1
6281560 Allen et al. Aug 2001 B1
6291305 Huang et al. Sep 2001 B1
6392524 Biegelsen et al. May 2002 B1
6404317 Mizoguchi et al. Jun 2002 B1
6414564 Mizoguchi et al. Jul 2002 B1
6433299 Varshney Aug 2002 B1
6441715 Johnson Aug 2002 B1
6452247 Gardner Sep 2002 B1
6583620 Honda et al. Jun 2003 B2
6593841 Mizoguchi et al. Jul 2003 B1
6597593 Cruz et al. Jul 2003 B1
6838863 Hazucha et al. Jan 2005 B2
6856228 Gardner Feb 2005 B2
6870456 Gardner Mar 2005 B2
6891461 Gardner May 2005 B2
7208963 Schrom et al. Apr 2007 B2
7852185 Gardner et al. Dec 2010 B2
8134548 Schrom et al. Mar 2012 B2
8471667 Gardner et al. Jun 2013 B2
20010052837 Walsh Dec 2001 A1
20030001709 Visser Jan 2003 A1
20030001713 Gardner Jan 2003 A1
20030122761 Hong Jul 2003 A1
20040070893 Ahn Apr 2004 A1
20040246226 Moon Dec 2004 A1
20060091896 Schrom et al. May 2006 A1
20070001762 Schrom et al. Jan 2007 A1
20110068887 Gardner et al. Mar 2011 A1
20120169425 Schrom et al. Jul 2012 A1
Foreign Referenced Citations (16)
Number Date Country
4117878 Dec 1991 DE
0295028 Dec 1988 EP
0725407 Aug 1996 EP
0884783 Dec 1998 EP
2369694 May 1978 FR
61020311 Jan 1986 JP
3214411 Sep 1991 JP
5081615 Apr 1993 JP
6124843 May 1994 JP
7272932 Oct 1995 JP
2000082621 Mar 2000 JP
378417 Jan 2000 TW
386310 Apr 2000 TW
411481 Nov 2000 TW
WO-0139220 May 2001 WO
WO-02065492 Aug 2002 WO
Non-Patent Literature Citations (35)
Entry
“Taiwanese Application Serial No. 93107741, Notice of Allowance mailed Apr. 29, 2010”, 3 pgs.
“Taiwanese Application Serial No. 93111253, Office Action received Mar. 22, 2006”, 2 pgs.
“Taiwanese Application Serial No. 93111253, Response filed Jun. 1, 2006 to Office Action received Mar. 22, 2006”, 9 pgs.
Baba, M., “GHz-Drive Magnetic Thin-Film Inductor Using CoNbZr Film”, Journal of the Magnetics Society of Japan, 24(4-2), (2000), 879-882.
Brandon, E., “Microinductors for Sacecraft Power Eectronics”, 6th International Symposium, Magnetic Materials, Processes and Device VI Applications to Storage and Microelectromechanical systems (MEMS), vol. 2000-29, The Electrochemical Society, Inc., Pennington, New Jersey, (2001), 559-567.
Fessant, A., et al., “Influence of In-Plane Anisotropy and Eddy Currents on the Frequency Spectra of the Complex Permeability of Amorphous CoZr Thin Films”, IEEE Transactions on Magnetics, 29(1), (Jan. 1993), 82-87.
Gardner, D., “High Frequency (GHz) and Low Resistance Integrated Inductors Using Magnetic Materials”, Proceedings of the IEEE 2001 International Interconnect Technology Conference, (Jun. 2001), 101-103.
Gardner, D. S., “Integrated Transformer”, U.S. Appl. No. 09/813,496, filed Mar. 21, 2001, 51 pgs.
Gardner, D. S., “Integrated Transformer”, U.S. Appl. No. 09/853,370, filed May 11, 2001, 62 pgs.
Gardner, D., “Mechanical Stress as a Function of Temperature for Aluminum Alloy Films”, Journal of Applied Physics, 67(4), (Feb. 15, 1990), 1831-1845.
Kobayashi, Y, “New Type Micro Cloth-Inductor and Transformer With Thin Amorphous Wires and Multi-Thin Coils”, IEEE Transactions on Magnetics, 28(5), (Sep. 1992), 3012-3014.
Koniklijke Philips Electronics, “Current Sensing Power MOSFETs Rev 01.00-09”, (Sep. 9, 2004).
Korenivski, V., “Magnetic Film Inductors for Radio Frequency Applications”, Journal of Applied Physics, 82(10), (Nov. 15, 1997), 5247-5254.
Long, J., “The Modeling, Characterization, and Design of Monolithic Inductors for Silicon RF IC's”, IEEE Journal of Solid-State Circuits, 32(2), (Mar. 1997), 357-369.
Matsuki, H., “A New Cloth Inductor Using Amorphous Fiber”, IEEE Transactions on Magnetics, 21(5), (Sep. 1985), 1738-1740.
Matsumoto, S., “Integration of a Power Supply for System-on-Chip”, IEICE Transactions on Fundamentals of Electronics, Communications and Computer Sciences, vol. E80-A, No. 2, (Feb. 1997), 276-282.
Mino, M., et al., “A New Planar Microtransformer for Use in Micro-Switching Converters”, IEEE Transactions on Magnetics, 28(4), (Jul. 1992), 1969-1973.
Mino, M., et al., “Planar Microtransformer With Monolithically-Integrated Rectifier Diodes For Micro-Switching Converters”, IEEE Transactions on Magnetics, vol. 32(2), (Mar. 1996), 291-296.
Mohan, S., “Bandwidth Extension in CMOS With Optimized On-Chip Inductors”, IEEE Journal of Solid-State Circuits, 35(3), (2000), 346-355.
Mohan, S., “Simple Accurate Expressions for Planar Spiral Inductances”, IEEE Journal of Solid-State Circuits, 34(10), (Oct. 1999), 1419-1424.
Niknejad, A., “Analysis, Design, and Optimization of Spiral Inductors and Transformers Si RF IC's”, IEEE Journal of Solid-State Circuits, 33(10), (Oct. 1998), 1470-1481.
O'Donnell, T., “Microtransformers and Inductors using Permalloy Thin Films”, Preparation, Properties, and Applications of Thin Ferromagnetic Films, http://www.iemw.tuwien.ac.at/publication/workshop0600/ODonnell.html, (Jun. 2000), 45-52.
Oshiro, O., et al., “A Novel Miniature Planar Inductor”, IEEE Transactions on Magnetics, vol. Mag-23, No. 5, (1987), 3759-3761.
Park, J. Y., et al., “Batch-Fabricated Microinductors With Electroplated Magnetically Anisotropic and Laminated Alloy Cores”, IEEE Transactions on Magnetics, 35(5), (Sep. 1999), 4291-4300.
Sato, T., “New Applications of Nanocrystalline Fe(Co—Fe)Hf—O Magnetic Films to micromagnetic devices”, Journal of Applied Physics, 83(11), (Jun. 1, 1998), 6658-6660.
Shirakawa, K., “Thin Film Cloth-Structured Inductor for Magnetic Integrated Circuit”, IEEE Transactions on Magnetics, 26(5), (Sep. 1990), 2262-2264.
Tomita, H., “Oblique-field annealing effect for in-plane magnetic anisotropy of soft magnetic Co—Nb—Zr thin films”, IEEE Transactions on Magnetics, 30(3), (May 1994), 1336-1339.
Yabukami, S., “Noise Analysis of a MHz-3 GHz Magnetic Thin Film Permeance Meter”, Journal of Applied Physics, 85(8), (Apr. 15, 1999), 5148-5150.
Yamaguchi, M., “1 GHz-drive magnetic thin-film inductors for RF integrated circuits using micro-patterned granular film”, Digest of INTERMAG 99. 1999 IEEE International Magnetics Conference, 1999, (May 18-21, 1999), ED01-ED01.
Yamaguchi, M., “Chapter 5. Magnetic Films for Planar Inductive Components and Devices”, In: Handbook of Thin Film Devices, vol. 4—Magnetic Thin Film Devices, Francombe, M. H., Editor, (2000), 185-212.
Yamaguchi, M., “Characteristics of Magnetic Thin-Film Inductors at Large Magnetic Field”, IEEE Transactions on Magnetics, 31(6), (Nov. 1995), 4229-4231.
Yamaguchi, M., “Magnetic Thin-Film Inductor for RF Integrated Circuits”, Extended Abstracts of the 1999 International Conference on Solid-State Devices and Materials, Tokyo, (1999), 580-581.
Yamaguchi, M., “Microfabrication and Characteristics of Magnetic Thin-Film Inductors in the Ultra High Frequency Region”, Journal of Applied Physics, 85(11), (Jun. 1, 1999), 7919-7922.
Yue, C., “On-Chip Spiral Inductors With Patterned Ground Shields for Si-Based RF IC's”, IEEE Jorunal of Solid-State Circuits, 33(5), (May 1998), 743-752.
Zommer, N., et al., “Power current mirror devices and their applications”, Proc. Power convers. Int. Conf. Jun. 1986, (1986), 275-283.
Related Publications (1)
Number Date Country
20130271105 A1 Oct 2013 US
Divisions (1)
Number Date Country
Parent 11173760 Jun 2005 US
Child 13417763 US
Continuations (1)
Number Date Country
Parent 13417763 Mar 2012 US
Child 13914358 US