Current measuring structure for testing integrated circuits

Abstract: A measuring structure comprising a first resistor (6) for converting a current to be measured into a voltage, and an operational amplifier (5) for measuring the current. A second resistor (10), series connected to and integrated with the first resistor (6), is activated by an input terminal (13) solely at the wafer testing stage, so as to reduce, in relation to the nominal value, the current corresponding to a predetermined voltage value detected by the operational amplifier, and enable optimum correlation of the reduced current value obtainable during wafer testing and the corresponding nominal current value.

Description: The present invention relates to a current measuring structure for testing integrated circuits. Integrated circuits are tested at various stages in the course of production, which tests include wafer testing (often referred to as EWS - Electrical Wafer Sort) in which the whole wafer (semiconductor slice in which various devices are integrated) is tested prior to separating the chips; and final testing of the separate chips mounted in the respective packages. In the case of power integrated circuits, the wafer test provides, among other things, for measuring various high currents, which are subsequently related to similar currents measured at the final test stage. A typical example is measurement of the current value triggering the current limiting circuit with which the power stages are normally provided. The above measurement is critical as regards both forcing of the current and acquisition of the measuring data, due to the high-energy voltage peaks ("spikes") produced by high currents in the presence of parasitic inductance caused by the measuring devices. Moreover, at the high current levels involved, the pad sensors are subject to severe wear, thus resulting in gradual aging of the measurement with time; and, finally, problems are encountered in relating the wafer and final test measurements, due to differing power dissipation conditions. To reduce the criticality of the measurement and so overcome the aforementioned drawbacks, a known practice when wafer testing is to measure a current lower than but related to the normal operating current. To demonstrate this approach, Fig.1 shows a known solution relative to a power stage with a d.c. current limiting circuit (the following account also applies to other solutions featuring switch-operated limiting circuits, by virtue of both types being based on current-voltage conversion by a calibrated resistor for generating a voltage proportional to the current through the power stage). In Fig.1, both the power stage and limiting circuit are shown schematically. More specifically, the power stage, indicated as a whole by 1 and forming part of integrated circuit 1a, is represented by a power MOS transistor 2 supplied at the drain terminal by current source 3; and the limiting stage, indicated by 4, comprises an operational amplifier 5, the output of which is connected to the drain terminal of transistor 2 (for limiting the current supplied to transistor 2), and the two inputs of which are connected to the two terminals of a sensing resistor 6 series connected to the source terminal of transistor 2. In particular, the negative input of amplifier 5 is connected to the common node between the drain terminal of transistor 2 and a first terminal of resistor 6; and the positive input of amplifier 5 is connected to the other terminal of resistor 6 through a voltage source 7 supplying voltage V R . Resistor 6 of limiting circuit 4 normally consists of a suitably sized metal strip, and presents an accurately known resistance R s normally ranging between a few tens and a few hundred mΩ, for reducing both power dissipation and the voltage drop in series with the power stage, so that voltage drop V 1 at the terminals of resistor 6 is generally in the order of a hundred mV at most. In the Fig.1 circuit, limiting stage 4 is operated when V 1 ≈ V R , i.e. when current I L through transistor 2 (and consequently resistor 6) equals: I L = V R /R s One technique for determining operation of the limiting circuit at less than nominal current (during normal operation of the integrated circuit) consists in reducing voltage V R supplied by source 7 at the wafer test stage as e.g. known from US-A-3 772 595. Such a reduction, which may be achieved in various ways (not described herein, by virtue of not forming part of the present invention), presents several basic drawbacks affecting correct correlation of the wafer and final test measurements, and thus resulting in problems in terms of electrical yield. The major problem posed by the above approach involves the voltage offset of operational amplifier 5. In fact, for obtaining a limit current for wafer testing, reduced by a scaling factor of, say, 10 in relation to the nominal value, by virtue of (1), V R must also be reduced by the same scaling factor to obtain values in the order of about ten mV. As the operational amplifiers normally employed for such applications present an offset of 1-2 mV, an excessively high measuring spread of 10-20% results, so that the above known approach is only feasible in the case of very low scaling factors, thus reducing the advantages to be gained. What is more, as the V R reduction factor increases, measuring repeatability decreases, by virtue of a reduction in V R emphasizing inaccuracy due to noise. It is an object of the present invention to provide a current measuring structure for testing integrated circuits, designed to overcome the aforementioned drawbacks typically associated with known solutions, and which provides for sufficiently reliable, accurate testing and correlation for determining the efficiency of the integrated circuit. According to the present invention, there is provided a current measuring structure for testing integrated circuits, as claimed in Claim 1 and in Claim 10 respectively. Therefore, instead of reducing the voltage drop at which the limiting circuit is activated, the current/voltage conversion resistance is increased by means of a resistive element formed in the integrated circuit and series connected to the current/voltage resistor, and which is activated during testing. A preferred non-limiting embodiment of the present invention will be described by way of example with reference to the accompanying drawings, in which: Fig.1 shows a simplified circuit diagram of a power stage with a known current limiting circuit; Fig.2 shows an equivalent circuit diagram of the structure according to the present invention applied to the known limiting circuit; Fig.3 shows a top plan view of the Fig.2 structure as implemented. As shown in Fig.2, in which any parts similar to those in Fig.1 are indicated using the same numbering system, the positive input of operational amplifier 5 is again connected to one terminal 6a of sensing resistor 6, while the negative input is connected to the other terminal 6b of resistor 6 via a second resistor 10 also indicated as a sensing resistor for wafer testing and presenting a resistance R sl . Terminal 6a of sensing resistor 6 is also connected to the drain terminal of transistor 2, while terminal 6b is connected to input terminal 12 of the integrated circuit. The negative input of operational amplifier 5 connected to terminal 10a of resistor 10 is also connected to a second input terminal 13 of the integrated circuit. According to the present invention, resistors 6 and 10 are integrated in the same integrated circuit 1a, and formed contiguously using the same technology, as shown in detail in Fig.3, which shows a metal strip 15 on the substrate 16 in which circuit 1a, and more specifically transistor 2 and operational amplifier 5 (shown only schematically), is integrated. A portion of strip 15 forms sensing resistor 6 of limiting circuit 4; and strip 15 is connected at one end to the drain terminal of transistor 2 (as shown schematically), and at the other end to a pad 17 defining input terminal 12 and to which is applied a probe (not shown) for measuring current I L2 through transistor 2 at the final test stage. From the end of metal strip 16 connected to pad 17 (terminal 6b), there extends a further suitably sized metal strip 18, one portion of which defines sensing resistor 10 for wafer testing. Metal strip 18 terminates at a second pad 19 smaller than pad 17 and defining input terminal 13 to which a probe is applied for measuring current I L1 through transistor 2 at the wafer test stage. Wafer test pad 19 is also connected by a metal connecting line 20 to the negative input of operational amplifier 5 (shown only schematically), the positive input of which is connected to metal strip 18 by metal connecting line 21 and through voltage source 7 (shown only schematically). In the integrated circuit, resistor 10 provides for three functions: when wafer testing, it acts as a sensing resistor for detecting the current through transistor 2; in other situations, it provides for modulating the current through terminal 12; and, in all other situations, it simply provides for connecting the negative input of operational amplifier 5 to resistor 6. In the first case (when wafer testing), pad 19 is connected to a measuring probe; in the second case, pad 19 is connected to appropriate circuit elements (for supplying variable current) so as to affect the value of the current through resistor 6; and, in the third case, pad 19 remains floating. When wafer testing, therefore, current I L1 through transistor 2 and terminal 13 flows through both resistors 6 and 10, and the intervention condition of the limiting loop corresponds with a current I L1 value of: I L1 = V R /R s +R s1 ) as shown in Fig.2. When final testing, on the other hand, terminal 13 is left floating; no current, other than the negligible input current of operational amplifier 5, flows through resistor 10; the current/voltage conversion required for testing is performed solely by resistor 6; and the intervention condition of the limiting loop is reached when the current through transistor 2 and measured at terminal 12 presents a value of: I L2 = V R /R s As such, the ratio between the nominal intervention currents measured respectively at the final and wafer test stages is determined by the following scaling factor K: K = I L2 /I L1 = (R s +R s1 )/R s which, by appropriately sizing R s1 , easily provides for achieving scaling factors as high as 10-15. The advantages of the structure according to the present invention will be clear from the foregoing description. In particular, it provides for achieving a scaling factor sufficient for the specific purpose in question, thus eliminating any drawbacks posed by comparable current measurements at the wafer and final test stages, and so reducing the criticality of the measurement and wear of the probes, and providing for improved correlation. As regards correlation, in particular, this is extremely good by virtue of depending solely on the type and repeatability of the manufacturing process and, in particular, on the matching of resistors 6 and 10. Formation of the resistors contiguously and at the same manufacturing stage therefore provides for excellent matching, with no particular electrical or layout provisions required. In actual practice, even for high scaling factors (10-15), mismatching, mainly for phototechnical reasons, has been estimated at about a few percent. Manufacture of the structure and related circuits is therefore straightforward and economical by virtue of involving no special machinery or technology. Finally, the structure according to the present invention may be employed for additional functions during normal operation of the circuit in which it is integrated, e.g. for modulating current supply to terminal 12, as already stated. To those skilled in the art it will be clear that changes may be made to the structure as described and illustrated herein without, however, departing from the scope of the present claims.

Claims: A current measuring structure for testing integrated circuits, said structure comprising a current sensor having an electric resistance and through which the current to be measured is supplied; and current measuring means (5) connected to said sensor and generating an electric signal related to said current; characterized by the fact that it comprises means (10, 12, 13) for varying the electric resistance of and integrated with said sensor. A structure as claimed in Claim 1, wherein said electric resistance of said sensor comprises a first resistive element (6); characterized by the fact that said varying means comprise a second resistive element (10) series connected to said first resistive element (6); and means (12) for bypassing said second resistive element (10) in predetermined operating conditions. A structure as claimed in Claim 2, characterized by the fact that said first and second resistive elements (6, 10) each comprise a first and second terminal (6a, 6b, 10a), said first terminals (6b) of said first and second resistive elements being mutually connected; and by the fact that said bypass means comprise a first contact element (12, 17) connected to said first terminals (6b) of said first and second resistive elements; and a second contact element (13, 19) connected to said second terminal (6b) of said second resistive element. A structure as claimed in Claim 3, characterized by the fact that said first and second resistive elements (6, 10) are each formed from a respective strip of resistive material (15, 18) having a first and second end corresponding with said first and second terminals (6b, 10a); said first ends of said strips of conducting material (15, 18) being contiguous. A structure as claimed in Claim 4, characterized by the fact that said strips of resistive material comprise metal strips (15, 18) on a substrate (16) of semiconductor material, and by the fact that said first and second contact elements each comprise a respective pad (17, 19). A structure as claimed in Claim 5, characterized by the fact that said metal strips (15, 18) are formed from a single layer of metal material. A structure as claimed in any one of the foregoing Claims from 3 to 6, characterized by the fact that said measuring means (5) present a first and second input connected to a respective said second terminal (6a, 10a) of said resistive elements (6, 10). A structure as claimed in Claim 7, characterized by the fact that said measuring means comprise an operational amplifier (5). A structure as claimed in Claim 1, characterized by the fact that said varying means comprise an input terminal (13) receiving an electric control signal for modulating said current to be measured. An integrated circuit (1a) comprising a component (2) supplied with a current to be measured; a current sensor (6) including a first resistive element and supplied with said current to be measured; and an operational amplifier element (5) connected to said current sensor and generating an output signal related to said current; characterized by the fact that it comprises a second resistive element (10) series connected to said first resistive element (6); said first and second resistive elements (6, 10) presenting a first common terminal (6b) and a second and third terminal (6a, 10a); said second terminal (6a) being connected to said component (2); and said second and third terminals (6a, 10a) being connected to respective inputs of said operational amplifier element (5); and by the fact that it comprises a first and second current forcing terminal (12, 13) connected respectively to said common terminal (6b) and to said third terminal (10a). Utilization of the current measuring structure, as claimed in claim 1, for modulating said current to be measured.

Inventors: PELLEGRINI FRANCO, PELLEGRINI, FRANCO
Applicants: ST MICROELECTRONICS SRL, STMICROELECTRONICS S.R.L.
Application year: 1992
Main classification: G01R31
IPC codes: H01L21, G01R31, G01R1