text: the swept frequency theft detection system of fig1 is , in part , like that shown and described in u . s . pat . no . 3 , 500 , 373 . as shown , there is provided a tuning oscillator 10 which produces a voltage whose amplitude varries at a given rate , e . g ., 300 cycles per second . this varying voltage is applied to a voltage tuneable swept radio frequency oscillator 12 which is designed to produce an output voltage which is nominally 2 megahertz ( mhz ). when the oscillator 12 is controlled by the tuning oscillator 10 however , its output frequency is swept between 1 . 95 mhz and 2 . 05 mhz at a 300 cycle per second rate . the swept frequency output of the oscillator 12 is supplied to a junction 14 ( see fig3 ) from which it branches to &# 34 ; lead &# 34 ; and &# 34 ; lag &# 34 ; phase shifts 16 and 18 . these phase shifters , which will be described in greater detail hereinafter in connection with fig3 act , respectively , to advance and retard the phase of the signals applied to them . in the case of the lead phase shifter 16 , the signal phase is advanced by approximately 45 °, while in the case of the lag phase shifter , the signal phase is retarded by approximately 45 °. there is thus produced a net phase differential of 90 ° at the outputs of the two phase shifters 16 and 18 . the output of the lead phase shifter 16 is applied to an amplifier 20 ; and the output of this amplifier is applied to a transverse antenna junction 22 . a transverse antenna winding 24 is connected to the junction 22 . the junction 22 is also connected to a first detector 26 ; and this is in turn connected to an alarm 28 . the output of the lag phase shifter 18 is applied to an amplifier 30 ; and the output of this amplifier is applied to a pair of lateral antenna junctions 32 and 34 . each of the detectors 26 and 40 ; and the alarm 28 may be constructed and arranged as described in connection with fig2 . as is there shown , the transverse antenna winding 24 comprises a multiturn coil lying in a plane which is substantially perpendicular to a path of egress ( indicated by an arrow a ) through a checkpoint . various physical means ( not shown ) are provided to confine the movement of protected articles , which are equipped with electronic responder circuits , so that they can exit from an enclosure only via the path shown by the arrow a . the protected article thus must pass either through or very near the transverse antenna winding 24 during egress from the enclosure . the two lateral antenna windings 36 and 38 also comprise multiturn coils . however these antennas are arranged on opposite sides of the egress path with their planes oriented parallel to the path and perpendicular to the plane of the transverse antenna winding 24 . as shown in fig2 all of the antenna windings have one end connected to ground . the opposite end of the transverse antenna winding 24 is connected to the junction 22 while the opposite end of the lateral antenna windings are connected to the junctions 32 and 34 . the system of fig1 and 2 operates to detect the presence of resonant responder circuits ( not shown ) carried on protected articles which pass through and by the antenna windings 24 , 36 and 38 along the egress path . the responder circuits are tuned to resonate at a frequency within the sweep range of the oscillator 12 . thus the responder circuits may be tuned to resonate at 2 mhz . when no responder circuit is present in the egress path , a relatively high impedance is presented to the antenna windings and most of the energy from the amplifiers 20 and 30 passes by the junctions 22 , 32 and 34 and becomes incident upon the detectors 26 and 40 . as long as a relatively constant energy level is applied to the detectors they do not produce any alarm actuating signal . when a responder circuit passes by or through the antenna windings , it resonates and absorbs energy each time the frequency of the oscillator 12 sweeps by the resonant frequency of the responder circuit . when the responder circuit is tuned to resonate at 2 mhz and the oscillator frequency sweep between 1 . 95 mhz and 2 . 05 mhz , this resonant response occurs twice during each sweep cycle or at a 600 response per second rate . the resonant responses cause a decrease in impedance in the vicinity of the antenna windings so that more of the transmitted energy passes out from the windings during the resonant response . this results in a decrease in the energy level applied to the detectors 26 and 40 . the detectors , as described in u . s . pat . no . 3 , 500 , 373 , are provided with special arrangements for detecting these energy decreases and for actuating the alarm 28 when they occur . the phase shifters 16 and 18 may be of any suitable construction which will produce a difference in phase between the lateral and transverse antenna windings . the particular phase shifter construction shown in fig3 has been found to be quite suitable for the present application . as shown in fig3 the lead phase shifter 16 comprises a resistor 42 connected in series between the junction 14 and the amplifier 20 . a capacitor 44 is connected across the resistor 42 . the lag phase shifter 18 comprises a resistor 46 connected in services between the junction 14 and the amplifier 30 . an inductor 48 and a capacitor 50 are together connected across the resistor 46 . it has been found that when the resistor 42 is about 680 ohms and the capacitor 44 is about 150 picofarads the lead phase shifter 16 will produce a phase shift of close to + 45 ° for frequencies in the range of 1 . 95 - 2 . 05 mhz . also when the resistor 46 is about 680 ohms and the inductor 48 is about 47 microhenries , the lag phase shifter will produce a phase shift of close to - 45 ° for frequencies in the range of 1 . 95 - 2 . 05 mhz . the capacitor 50 is used to prevent short circuiting of the resistor 46 by the inductor 48 ; and it has been found that this capacitor will serve this function without adversely affecting phase shift for the frequencies mentioned when its capacitance is approximately 0 . 1 microfarad . the phase shifters 16 and 18 may be adjusted to produce any differential in the net phase shift between the lateral and transverse antenna windings . however , as will be seen , a 90 ° net phase shift should produce a more uniform field distribution with the antenna arrangement of fig2 . also , it is not necessary that two separate phase shifters be used . a single phase shifter capable of producing a 90 ° phase shift in the signal to one of the amplifiers 20 or 30 would produce a similar result . the use of two phase shifters , each of which produces only a 45 ° phase shift , however , permits a more accurate phase shift over the frequency sweep range with less expensive construction . also it has been found that the frequency sensitivity of the two phase shifters 16 and 18 is complimentary during the 1 . 95 to 2 . 05 mhz frequency sweep . thus when the frequency at any instant is such that the lead phase shifter 16 produces less lead , that same frequency causes the lag phase shifter 18 to produce greater lag so that the net phase difference remains essentially the same as frequency shifts . the manner in which the above described antenna orientation and phase shifted antenna excitation serves to produce a revolving field which eliminates dead zones can be seen in a comparison of fig4 and 5 . fig4 and 5 each comprise a group of section views taken along line 4 -- 4 of fig2 . these section views sever the vertical portions of both the transverse and horizontal antenna windings 24 , 36 and 38 . thus there are shown severed ends of vertical portions 24a and 24b of the transverse antenna winding 24 , severed ends of the vertical portions 36a and 36b of the lateral antenna winding 36 and severed ends the vertical portions 38a and 38b of the lateral antenna winding 38 . as can be seen in fig2 when current flows upwardly in the vertical portion 24a , it flows downwardly in the opposite vertical portion 24b . this also applies to vertical portions 36a and 36b and 38a and 38b . reverse current flows occur , of course , during one half of each cycle of antenna energization . the flow of current through the various antenna windings is accompanied by a circular magnetic field surrounding the winding wires as illustrated by arrows b in fig4 and 5 . the direction of the various circular magnetic fields b corresponds to the direction of current flow through the winding which each field surrounds . thus , the direction of the circular magnetic field reverses itself upon each half cycle of antenna energization . the distribution of electromagnetic energy in the vicinity of the egress path a will now be described with regard to the magnetic fields b produced by currents in the antenna windings 24 , 36 and 38 . in the successive 90 ° intervals of antenna energization represented by fig4 a - d , each of the three antenna windings 24 , 36 and 38 is energized in phase , according to the prior art . thus all antenna windings conduct maximum current at the same time and all antenna windings conduct zero current at the next following 90 ° interval . the major direction of magnetic field strength , which is represented by an arrow c in fig4 is determined according to the mutual additive and subtractive effects of the circular magnetic fields b in the various antenna windings . as can be seen in fig4 a , the major magnetic field energization c is at an angle α with respect to the path a . after the next 90 ° interval the magnetic field energization diminishes to zero as shown in fig4 b . thereafter as shown in fig4 c , the major magnetic field energization c is again at the angle α with respect to the egress path a , but is reversed in direction . finally , as shown in fig4 d , after the last 90 ° interval the magnetic field strength again diminishes to zero . it will be appreciated from fig4 that the major magnetic field strength c always lies along a path which crosses the egress path a at an angle α . also by considering the additive and subtractive effects of the circular magnetic fields b within the various quadrants ( a ), ( b ), ( c ) and ( d ), it will be seen that a minimum magnetic field strength is always present in quadrants ( b ) and ( d ) while maximum magnetic field strength is present only in quadrants ( a ) and ( c ). thus , by taking care to traverse the checkpoint along a path indicated by the dashed arrow d , one can cross the path of maximum field strength at substantially a right angle to it and thereby minimize the duration required to pass through the high intensity region of the field . also , by following the path of the arrow d , one will traverse the checkpoint via the quadrants ( b ) and ( d ) of minimum field energization . these quadrants make up dead zones within which only minimal response can be obtained from a rebroadcaster circuit . as a result a possibility exists in this prior art arrangement , for a protected article to pass through a checkpoint undetected if it follows a particular path . turning now to fig5 wherein operation according to the present invention is shown , it will be seen that the transverse antenna winding 24 is energized at a 90 ° phase relationship to the energization of the lateral antennas 36 and 38 . as can be seen in fig5 a , when maximum current flows through the lateral antenna windings 36 and 38 , no current flows through the transverse antenna winding 24 . the additive and subtractive effects of the circular magnetic fields b are such that they produce a net maximum magnetic field energization c which is at a right angle β to the egress path a . after the next 90 ° interval , as seen in fig5 b , the current through the lateral antenna windings 36 and 38 diminishes to zero and the current through the transverse antenna winding 24 becomes maximum . the net effect is to swing the maximum magnetic field energization c into alignment with the egress path a . thereafter , after the next 90 ° interval of antenna energization , as shown in fig5 c , current in the transverse antenna winding 24 diminishes to zero while current through the lateral antenna windings 36 and 38 again reaches maximum in the opposite direction from that shown in fig5 a . this causes the maximum magnetic field energization c to swing further around until it again is at a right angle β to the egress path a . finally after the last 90 ° interval of antenna energization , as seen in fig5 d , the circular magnetic fields b cause the maximum magnetic field energization to swing back along the egress path direction a . it will be appreciated that by interpolation it can be shown that the maximum magnetic field vector c revolves circularly during antenna energization . thus any dead zones are swept around and the entire vicinity of the egress path a is electromagnetically energized uniformly . further , since the electromagnetic field pattern moves continuously there is no path along which one may pass in which the magnetic field strength is always minimal . thus there is provided a means for improving the detection reliability of responder circuits in electronic theft detection system . while the invention has been described with reference to the preferred form thereof , it will be obvious to those skilled in the art to which the invention pertains , after understanding the invention , that various changes and modifications may be made therein without departing from the spirit and scope of the invention , as defined by the claims appended hereto .