This invention relates to temperature coefficient factor circuits which are current or voltage sources which deliver a current or a voltage which varies with temperature according to a temperature coefficient factor (TCF). This invention further relates to semiconductor devices, and radar devices.
An operation of specific electronic circuits may vary together with variations of the temperature of the electronic circuit. Transistors and diodes junctions have a current/voltage relationship that varies with temperature. The variations may introduce uncertainties in the operation of the electronic circuits and may degrade the performance of the electronic circuits. Besides transistors and diodes, other parts of the electronic circuits may also be subject to operational variations in dependency of the temperature of the parts. Thus, there is a need for compensating the operation of these devices for temperature variations.
In many circuits voltage references and/or current references are used as a basic fundamental sub-circuit. Many of those current and voltage references are designed to be temperature independent, however, if they provide a well-defined temperature dependent current of voltage, their temperature dependency may be used to compensate for temperature effects in other parts of the circuitry.
The term Temperature Coefficient Factor (TCF) is introduced in this context and it is being used to refer to a slope of a current provided by a current source when the temperature varies. The unit of TCF is ppmK, which means, if the temperature changes with 1 K, the current provided by the current source varies with 1·10−6 A. A temperature compensation circuitry provides, preferably, a current with a well-defined TCF. In literature many examples of TCF circuits are provided which have such a well-defined TCF. In a number of applications, such as, for example, in radar applications, it is desired to have a current source which provides a current with a programmable TCF. Thus, it is required to have a specific TCF in response to a control signal. Traditional approaches are to manufacture a plurality of current sources with different TCF values and only switch on a specific one of the plurality of current sources in dependence of the control signal. Such a programmable TCF circuit requires a lot of circuitry to be manufactured on, for example, an integrated circuit and is, thus, relatively expensive.
In document U.S. Pat. No. 6,222,470 discloses a digitally programmable temperature coefficient factor (TCF) circuit. The circuit provides a reference current or a reference voltage which value varies with temperature in dependence of a programmable TCF. The reference voltage is obtained by providing the reference current to a resistor. The reference current is a summation of a first current and a second current. The first current has a programmable value and is a programmable portion of a first maximum current I1max which has a well-defined TCF. The second current has a programmable value and is a programmable portion of a second maximum current I1ma, which does not vary with temperature. The first current is generated by a first Digital-to-Analog-Converter circuit (DAC) which receives the first maximum current with the well-defined TCF and which receives a first digital signal. The first DAC divides the first maximum current in dependence of the first digital signal. The first digital signal may have a maximum value N1max, and the actual value N1, and the DAC divides the first maximum current by the ratio N1/N1max. Thus, the first current has the value (N1/N1max)-Imax,which implies that the TCF of the first current also varies with the value of N1. In this manner the TCF of the reference current provided by the circuit also varies with the value of N1. It is to be noted that the generation of second current is performed in an equal manner, with a second DAC. The value of the second current varies with a value N2, however, it has a TCF of about 0.
The cited patent U.S. Pat. No. 6,222,470 only discloses that the first current, which varies with a programmable TCF, is generated with a DAC. The patent remains silent about the specific implementation of this DAC. Based on the disclosure of document, it may be concluded that if the TCF of the first maximum current is positive, the circuitry of U.S. Pat. No. 6,222,470 can only generated reference currents with a positive first maximum current, which is in specific applications a major limitation. Further, although the implementation of the DAC's is not disclosed, it is expected that when they have to be implemented on silicon, they are a relatively large and, thus, expensive circuit.
The present invention provides a temperature coefficient factor circuit, a semiconductor device, and a radar device as described in the accompanying claims.
Specific embodiments of the invention are set forth in the dependent claims.
These and other aspects of the invention will be apparent from and elucidated with reference to the embodiments described hereinafter.
Further details, aspects and embodiments of the invention will be described, by way of example only, with reference to the drawings. Elements in the figures are illustrated for simplicity and clarity and have not necessarily been drawn to scale.
The first current source 102 provides, in operation, a first current Ipos which varies with the temperature according to a first temperature coefficient factor TCFpos which has a positive value. The second current source 110 provides, in operation, a second current Ineg which varies with the temperature according to a second temperature coefficient factor TCFneg which has a negative value.
The first programmable amplifying current mirror PACM1 receives the first current Ipos, receives a control signal ctrl and is coupled to the common terminal 112. The first programmable amplifying current mirror PACM1 conducts a first amplified current A·Ipos to the common terminal 112. The received first current Ipos is amplified towards the first amplified current A·Ipos according to a first amplification factor A. The first amplification factor A is adapted in dependence of the control signal ctrl.
The second programmable amplifying current mirror PACM2 receives the second current Ineg, receives the control signal ctrl and is coupled to the common terminal 112. The second programmable amplifying current mirror PACM2 conducts a second amplified current B·Ineg away from the common terminal 112. The received second current Ineg is amplified towards the second amplified current B·Ineg according to a second amplification factor B. The second amplification factor B is adapted in dependence of the control signal ctrl.
The output current circuit IOUTC, 106 is coupled to the common terminal 112 and conducts a difference current Idiff away from the common terminal 112. The difference current Idiff is substantially equal to the first amplified current A·Ipos minus the second amplified current B·Ineg. The output current circuit IOUTC, 106 provides, in operation, an output current Iout which varies with a required temperature coefficient factor TCFwanted The output current Iout is based on the difference current.
The operation of the circuit is explained on basis of a mathematical deduction:
It is known that:
The derivative of (2) with respect to T is:
When (1) and (3) are combined, and when it is assumed that Iout=Idiff, one gets:
Idiff·TCFwanted=A·Ipos·TCFpos−B·Ineg·TCFneg (4)
If one assumes that Ipos=Ineg=I, and Idiff is replaced by (2) in formula (4), and the result is rewritten to, one gets:
Thus, formula (5) shows that the TCF of the output current is a combination of the TCF of the first current source and the TCF of the second current source and that the TCF of the output current depends on the TCF of the first current source and of the
second current source by the amplification factors A and B.
If it is assumed that
and formula (5) is rearranged, one gets:
Thus, with formula (6) R can be calculated and subsequently the amplification factors A and B may be chosen such that the ratio of the chosen amplification factor A and B are close the ratio R which is calculated with formula (6).
In a practical embodiment, the control signal comprises information about the wanted TCF TCFwanted, the TCF of the first current course TCFpos, and the TCF of the second current source TCFneg. Subsequently, a controller of the first programmable amplifying current mirror PACM1 calculates a value R, selects values A and B, and uses the value A as it's amplification factor. A controller of the second programmable amplifying current mirror PACM2 calculates a value R, selects values A and B, and uses the value B as it's amplification factor. The second programmable amplifying current mirror PACM2 selects the values A and B in the same manner as the first programmable amplifying current mirror PACM1. The selected values A and B results in a value
which is approximately the value R of formula (6). In an embodiment, the value Rselected does not deviate more than 10% from the calculated value R of formula (6). In an embodiment, the value Rselected does not deviate more than 5% from the calculated value R of formula (6). In another embodiment, the first programmable amplifying current mirror PACM1 and the second programmable amplifying current mirror PACM2 have the capability to only use an amplification factor from a predefined set of amplification factors A1 . . . An, Bi . . . Bm and from this predefined set of amplification a combination of one Ax amplification factor and one By amplification factor is selected such that the
is closed to the ration R calculated by formula (6) and such that other factors based on other selections are less close to the ratio R calculated by formula (6).
It is to be noted that it is assumed in the previous paragraph that the TCF of the first current source and of the second current source have a fixed value. However, in general, the embodiments falling within the scope of the invention of this application are not limited to first current source and of the second current source have a fixed TCF. In specific embodiments the TCF of the first current source and of the second current source may be changed to a required value.
In an example: Assume that the TCF of the first current source is TCFpos=3504 ppmK and the TCF of the second current source is TCFneg=−1450 ppmK. These values may be the result of a specifically designed current source and may be measured after manufacturing the respective current source. If, for example, the required TCF of the output current TCFwanted=4500 ppmK, than the ratio R, calculated with formula (6) is R=5.97. If the first amplification factor is chosen to be A=6 and if the second amplification factor is chosen to be B=1, than, the selected ratio Rselected=6, which is relatively close to the calculated value. Thus, the first programmable amplifying current mirror PACM1 amplifies current Ipos with a factor 6, and the second programmable amplifying current mirror PACM2 amplifies current Ineg with a factor 1.
In summary,
The first programmable amplifying current mirror 104 comprises a first controller CTRL1, 202, a first MOS transistor P1 and a plurality of parallel arranged first mirror MOS transistor P2 . . .P4. The first MOS transistor P1 and the plurality of parallel arranged first mirror MOS transistor P2 . . . P4 are all of P-type, and that they have similar characteristics (such as gate width and length). The first MOS transistor P1 is arranged with its source-drain current conduction path in the current path of the current delivered by the first current source 102. A drain of the first MOS transistor P1 is coupled to a gate of the first MOS transistor P1. Each one of the plurality of parallel arranged first mirror MOS transistor P2 . . . P4 may be coupled with its gate, via a controllable switch SW1 . . . SW3 to the gate of the first MOS transistor P1. If such a first mirror MOS transistor is coupled to the gate of the first MOS transistor P1, it forms together with the first MOS transistor P1 a current mirror circuit and, if the first current Ipos=I1 flows through the first MOS transistor P1, the same first current flows through the first mirror MOS transistor P2 . . . P4 which are coupled with its gate to the gate of the first MOS transistor P1. The first mirror MOS transistors P2 . . . P4 are coupled with a controllable switch SW1′ . . . SW3′ to the common node 112. Each one of the controllable switches SW. . . SW3 forms a pair with a corresponding controllable switch SW1′ . . . SW3′. If one of the controllable switches SW1 . . . SW3 is closed, the corresponding controllable switch SW1′. . . SW3′ is closed such that the mirrored first current provided by a specific one of the first mirror MOS transistor P2 . . . P4 is conducted towards the common node 112. If, for example, controllable switch pair SW1-SW1′ and controllable switch pair SW2-SW2′ are closed and controllable switch pair SW3-SW3′ is not closed, two times the current is provided to the common node 112, and, thus, the amplification factor of the first programmable amplifying current mirror 104 is A=2. The first controller ctrll is configured to close or open the controllable switch pairs SW1-SW1′ SW3-SW3′ in dependence of the control signal ctrl. As discussed in the context of
The second programmable amplifying current mirror 108 comprises a second controller CTRL2, 204, a second MOS transistor N1 and a plurality of parallel arranged second mirror MOS transistor N2 . . . N4. The second MOS transistor N1 and the plurality of parallel arranged second mirror MOS transistor N2 . . . N4 are all of an N-type, and that they have similar characteristics (such as gate width and length). The second MOS transistor N1 is arranged with its source-drain current conduction path in the current path of the current delivered by the second current source 110. A drain of the second MOS transistor N1 is coupled to a gate of the second MOS transistor N1. Each one of the plurality of parallel arranged second mirror MOS transistor N2 . . . N4 may be coupled with its gate, via a controllable switch SW4 . . . SW6 to the gate of the second MOS transistor N1. If such a second mirror MOS transistor is coupled to the gate of the second MOS transistor N1, it forms together with the second MOS transistor N1 a current mirror circuit and, if the second current Ineg=I2 flows through the second MOS transistor N1, the same second current I2 flows through the second mirror MOS transistor N2 . . . N4 which are coupled with its gate to the gate of the second MOS transistor N1. The second mirror MOS transistors N2 . . . N4 are coupled with a controllable switch SW4′. . . SW6′ to the common node 112. Each one of the controllable switches SW4 . . . SW6 forms a pair with a corresponding controllable switch SW4′. . . SW6′. If one of the controllable switches SW4 . . . SW6 is closed, the corresponding controllable switch SW4′. . . SW6′ is closed such that the mirrored second current provided by a specific one of the second mirror MOS transistor N2 . . . N4 is conducted away from the common node 112. If, for example, controllable switch pair SW4-SW4′ and controllable switch pair SW5-SW5′ are closed and controllable switch pair SW6-SW6′ is not closed, two times the current I2 is conducted away from the common node 112, and, thus, the amplification factor of the second programmable amplifying current mirror 108 is B=2. The second controller ctrl2 is configured to close or open the controllable switch pairs SW4-SW4 ′ SW6-SW6′ in dependence of the control signal ctrl. As discussed in the context of
The output current circuit 106 receives the difference current Idiff and provides the output current Iout. It may be advantageous if the output current Iout has, except variations which depend on the temperature coefficient factor TCFwanted, a substantially constant value which does not depend on the amplification factors A and B. Namely, if we assume that the first current and the second current I2 are, except variations which depend on the temperature coefficient factor TCFpos and TCFneg, substantially equal to eachother, Idiff has the value: Idiff=A·I−B·I1 and, thus, the value depends on the amplification factor A and B. The output current circuit 106 is configured to divide the current Idiff with a divisor C such that the value of Iout, except variations of the value of this current which depend on temperature differences and different value for the temperature coefficient factor TCFwante, is substantially constant, and, in an embodiment, is substantially equal to the first current The divisor C has to be equal to A-B.
The output current circuit 106 comprises a plurality of parallel arranged output mirror MOS transistors N5 . . . N7, an output MOS transistor N8 and a third controller CTRL3, 206. The plurality of output mirror MOS transistors N5 . . . N7 and the output MOS transistor N8 are of the same type as the second MOS transistor N1 and the plurality of second mirror MOS transistor N2 . . . N4. The plurality of output mirror MOS transistor N5 . . . N7 are arranged in a parallel configuration and may be coupled with a corresponding controllable switch SW7 . . . SW9 in the current conduction path of the difference current Idiff. The difference current Idiff is subdivided over a number of output mirror MOS transistors N5 . . . N7 which are with the controllable switch SW7 . . . SW9 in the current conduction path of the difference current Idiff. Each one of the controllable switches SW7 . . . SW9 forms a pair with another controllable switch SW7′ . . . SW9′ which is arranged in an electrical coupling between a drain and a gate of its corresponding output mirror MOS transistor. The controllable switches SW7 . . . SW9-SW7′ . . . SW9′ are closed and opened pair-wise by the third controller. The gates of all output mirror MOS transistors N5 . . . N7 are coupled to a gate of the output MOS transistor N8, and thereby they form a current mirroring circuit. lf, for example, only the controllable switches of the pair SW7-SW7′ are closed, and the controllable switches of pairs SW8-SW8′ and SW9-SW9′ are opened, the current which flows through output mirror MOS transistor N5 is mirrored by output transistor N8 and, thus, Iout=Idiff. If, for example, the controllable switches of the pairs SW7-SW7′, SW8-SW8′ are closed, and the controllable switches of pair SW9-SW9′ are opened, a current which flows through output mirror MOS transistors is equal to Idiff2 and, consequently, the output current is Iout=Idiff/2. The output current Iout can be made substantially equal to the first current provided by the first current source 102 (if one assumes that the first current is substantially equal to the second current I2) if the number of MOS transistors which conduct a current towards the common terminal 112 is equal to the number of MOS transistors which conduct a current I2=I1 away from the common terminal. Thus, if the first programmable amplifying current mirror 104 closes A switch pairs, and the second programmable amplifying current mirror 108 close B switch pairs, the output current circuit has to close C=A-B switch pairs. It is to be noted that the output current circuit has to close at least one switch pair in order to be able to provide the output current Iout. Further, it is to be noted that A should always be larger than B. Thus, the third controller CTRL3, 206 receives a control signal crtl which comprises information an TCFpos, TCFneg and TCFwanted, and calculated, corresponding to the calculations performed by the first controller CTRL1, 202, the second controller CTRL2, 204, the values for A and B, and subsequently calculates C, and subsequently the third controller CTRL3, 206 closes a corresponding number of switch pairs SW7-SW7′ . . SW9-SW9′.
In an example, the temperature coefficient factor of the first current source is TCFpos=3500 ppmK and the temperature coefficient factor of the second current source is TCFneg=−1450, a number of TCFwanted can be created with the circuitry of
It is to be noted that Table 1 is based on the assumption that B is larger than 0, because otherwise the ratio R=A/B would result in an infinite large value, however, the practical implementation of the temperature coefficient factor may include controllers which chose B to be 0.
The example of
In
As discussed in the context of
Based on the teaching of
Furthermore, the second programmable amplifying current mirror and the output current circuit may be implemented in a similar way as the presented embodiment of first programmable amplifying current mirror 504 by creating transistor units which comprise 2n, with n=0 to e.g. 7, transistors. It is further to be noted that the number of transistors in a single transistor unit are not necessary limited to values which are a power of 2. Depending on the specific application one may select specific numbers of transistors in a transistor unit such that the current with required temperature coefficient factors may be created by the temperature coefficient factor circuit.
By using such flexible programmable amplifying current mirrors, the temperature coefficient factor is able to create currents which have a selected temperature coefficient factor which is selected from a relatively large set of possible temperature coefficient factors. Thus, the circuit provides an enormous flexibility. Further, the amount of MOS transistors used in the circuit is relatively low, especially when the number is compared to circuits in which a plurality of temperature coefficient factor circuits are arranged in parallel and in which only one of the plurality of temperature coefficient factor circuits is used to create a current with a specific temperature coefficient factor.
At the left end of
The first current path Ip1 comprises a series arrangement of a first bipolar npn transistor T1 and a first resistor R1. The first transistor T1 is coupled with its collector to the first current mirror circuit 602 (and, thus, to the drain of MOS transistor P13), with its emitter to the first resistor R1 and with its base to its emitter. The first resistor R1 is coupled in between the ground voltage Vgnd and the emitter of the first transistor T1. The second current path Ip2 comprises a second bipolar npn transistor T1 which has characteristics which are almost all equal to the characteristics of the first transistor T1, only transistor T1 has a larger emitter area and the ratio between the emitter area of T1 and the emitter area of T2 is N:1. The transistor T2 is coupled with its base to the base of the first transistor, with its collector to the first current mirror circuit 602 (and, thus, to the drain of MOS transistor P14) and with its emitter to the ground voltage Vgnd. The third current path Ip3 comprises a third transistor T3 which has characteristics which are equal to the characteristics of the second transistor T2. The third transistor T3 is coupled with its base to the collector of the second transistor T2, with its collector to the first current mirror circuit 602 (and, thus, to the drain and gate of MOS transistor P15), and with its emitter to the ground voltage Vgnd.
In the first current source 606 a base of the second transistor T2 receives a first base-emitter voltage Vbe1 and a base of the third transistor T3 receive a second base-emitter voltage Vbe2 plus a voltage which is formed by the current through the first current path Ip1 multiplied by the resistance of resistor R1. Thus, the base of the third transistor T3 receives a voltage Vbe2+Ip1·R1. The base-emitter voltage difference between T2 and T3 is ΔVbe and the voltage difference depends on temperature. In the circuit of
wherein k is the Boltzmann constant, q is the magnitude of the electrical charge on an electron, T is the temperature, and N is the value of N from the emitter-area ratio N:1 (wherein the emitter area of the first transistor T1 is divided by the emitter area of the second transistor T2). Consequently, the current flowing through the first current path, the second current path, the third current path and the output current path is equal to
In (N), wnerein R1 is the resistance of resistor R1.
Although not strictly necessary for the generation of the first current Ipos=I1, the feedback loop of the first current source comprises a series arrangement of a first stabilizing resistor Rz1 and a first stabilizing capacitor Cz1 which is coupled between the base of the third transistor T3 and the ground voltage Vgnd. Oscillations are prevented and the loop has a good phase and gain margin.
It is to be noted that, as described and claimed, the current paths are provided between the supply voltage Vd and the ground voltage Vgnd. It is assumed that the complete current flowing through, for example, MOS transistor P13 also flows through the first transistor T3 and the first resistor. The same applies to the second current path Ip2 and the third current path Ip3: currents through P14 and P15 also flow, respectively, through the second transistor T2 and the third transistor T3. In practice relatively small current flow also to the bases of the respective transistors and, thus, the current through MOS transistors P13 . . . P15 may slight deviate from current respectively through transistors T3 . . .T3.
A further advantage of the presented first current source 606 is that the first current source 606 also operates with a relatively small supply voltage Vd—often a much smaller supply voltage than known prior art current sources which provide a current varying with temperature. Additionally, the first current source 606 provides a current which has a good power supply rejection ration (PSRR), which means that, if the supply voltage Vd varies, the current Ipos=I1 provided by the first current source 606 does not vary much.
The first current source 606, as presented in
At the right end of
The fourth current path Ip4 comprises a second resistor R2. The second resistor R2 is coupled in between the second current mirror circuit 608 and the ground voltage Vgnd—in other words, the second resistor R2 is coupled in between the drain of MOS transistor P16 and the ground voltage Vgnd. The fifth current path Ip5 comprises a fourth bipolar npn transistor T4. The base of the transistor is coupled to a terminal shared by the second resistor R2 and the second current mirror circuit 608. The fourth transistor T4 is further coupled with its collector to the second current mirror circuit 608 (i.e. the drain of MOS transistor P17) and with its emitter to the ground voltage Vgnd. The sixth current path Ip6 comprises a fifth npn transistor T5 with characteristics which are equal to the characteristics of the fifth transistor T5. A base of transistor T5 is coupled to a terminal shared by the collector of the fourth transistor T4 and the second current mirror circuit 608, a collector of the fifth transistor T5 is coupled to the second current mirror circuit (i.e. the drain of MOS transistor P18), and an emitter of the fifth transistor T5 is coupled to the ground voltage Vgnd
The operation of the second current source 610 is as follows: the second resistor R2, the fourth transistor T4 and the fifth transistor T5 are arranged such that the current which flows through the different current paths Ip4, Ip5, Ip6,
varies with temperature according to a negative temperature coefficient factor. Taking the derivative of Ineg with respect to temperature results in
with F(T) a function of temperature. Even if the variation of Ineg is not a constant with regards to the temperature T, it is always a negative value.
Although not strictly necessary for the generation of the second current Ineg=I2, the feedback loop of the second current source comprises a series arrangement of a second stabilizing resistor Rz2 and a second stabilizing capacitor Czb 2 which is coupled between the base of the fifth transistor T5 and the ground voltage Vgnd. Oscillations are prevented and the loop has a good phase and gain margin.
A further advantage of the presented second current source 610 is that the second current source 610 also operates with a relatively small supply voltage Vd—often a much smaller supply voltage than known prior art current sources which provides a current varying with temperature. Additionally, the second current source 610 provides a current which has a good power supply rejection ration (PSRR), which means that, if the supply voltage Vd varies, the current Ineg=I2 provided by the second current source 610 does not vary much.
The second current source 610, as presented in
In the foregoing specification, the invention has been described with reference to specific examples of embodiments of the invention. It will, however, be evident that various modifications and changes may be made therein without departing from the broader spirit and scope of the invention as set forth in the appended claims. For example, the connections may be an type of connection suitable to transfer signals from or to the respective nodes, units or devices, for example via intermediate devices. Accordingly, unless implied or stated otherwise the connections may for example be direct connections or indirect connections. Furthermore, the meaning of the term “coupled” is broader than the term “connected”. When a first element is coupled to a second element, other elements may be in between the first element and the second element to provide the coupling. Between electrical elements being coupled to each other exists a direct or indirect voltage or current connection.
The conductors as discussed herein may be illustrated or described in reference to being a single conductor, a plurality of conductors, unidirectional conductors, or bidirectional conductors. However, different embodiments may vary the implementation of the conductors. For example, separate unidirectional conductors may be used rather than bidirectional conductors and vice versa.
Because the amplification stages and the wideband power amplifiers according to the present invention are, for the most part, composed of electronic components and circuits known to those skilled in the art, circuit details will not be explained in any greater extent than that considered necessary as illustrated above, for the understanding and appreciation of the underlying concepts of the present invention and in order not to obfuscate or distract from the teachings of the present invention.
Although the invention has been described with respect to specific conductivity types or polarity of potentials, skilled artisans appreciated that conductivity types and polarities of potentials may be reversed.
Those skilled in the art will recognize that the boundaries between logic blocks are merely illustrative and that alternative embodiments may merge logic blocks or circuit elements or impose an alternate decomposition of functionality upon various logic blocks or circuit elements.
Thus, it is to be understood that the architectures depicted herein are merely exemplary, and that in fact many other architectures can be implemented which achieve the same functionality. In an abstract, but still definite sense, any arrangement of components to achieve the same functionality is effectively “associated” such that the desired functionality is achieved. Hence, any two components herein combined to achieve a particular functionality can be seen as “associated with” each other such that the desired functionality is achieved, irrespective of architectures or intermedial components. Likewise, any two components so associated can also be viewed as being “operably connected,” or “operably coupled,” to each other to achieve the desired functionality.
However, other modifications, variations and alternatives are also possible. The specifications and drawings are, accordingly, to be regarded in an illustrative rather than in a restrictive sense.
In the claims, any reference signs placed between parentheses shall not be construed as limiting the claim. The word ‘comprising’ does not exclude the presence of other elements or steps then those listed in a claim. Furthermore, Furthermore, the terms “a” or “an,” as used herein, are defined as one or more than one. Also, the use of introductory phrases such as “at least one” and “one or more” in the claims should not be construed to imply that the introduction of another claim element by the indefinite articles “a” or “an” limits any particular claim containing such introduced claim element to inventions containing only one such element, even when the same claim includes the introductory phrases “one or more” or “at least one” and indefinite articles such as “a” or “an.” The same holds true for the use of definite articles. Unless stated otherwise, terms such as “first” and “second” are used to arbitrarily distinguish between the elements such terms describe. Thus, these terms are not necessarily intended to indicate temporal or other prioritization of such elements The mere fact that certain measures are recited in mutually different claims does not indicate that a combination of these measures cannot be used to advantage.
Filing Document | Filing Date | Country | Kind |
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PCT/IB2012/002670 | 11/7/2012 | WO | 00 |
Publishing Document | Publishing Date | Country | Kind |
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WO2014/072763 | 5/15/2014 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
5828329 | Burns | Oct 1998 | A |
6222470 | Schuelke | Apr 2001 | B1 |
7119528 | Rasmus | Oct 2006 | B1 |
7307468 | Vasudevan | Dec 2007 | B1 |
7839202 | Sengupta et al. | Nov 2010 | B2 |
20020109539 | Takeuchi et al. | Aug 2002 | A1 |
20030155650 | Moon et al. | Aug 2003 | A1 |
20050248330 | Lin et al. | Nov 2005 | A1 |
20080224761 | Deng et al. | Sep 2008 | A1 |
20110043185 | Kim | Feb 2011 | A1 |
20120056609 | Sato | Mar 2012 | A1 |
Entry |
---|
International Search Report and Written Opinion correlating to PCT/IB2012/002670 dated Aug. 21, 2013. |
Gunawan, Made et al; “A curvature-Corrected Low-Voltage Bandgap Reference”; IEEE Journal of Solid-State Circuits, vol. 28, No. 6; 4 pages (Jun. 1993). |
Deval, Y. et al; “1-Volt Ratiometric Temperature Stable Current Reference”; IEEE International Symposium on Circuits and Systems, Hong Kong; 4 pages (Sep. 6-Dec. 1997). |
Number | Date | Country | |
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20150309527 A1 | Oct 2015 | US |