a system in accordance with the invention , referring now to fig1 , is depicted in an example intended for use in hair removal , the treatment of spider veins and other skin disorders . this configuration includes a hand - held applicator that is suitable for potential use at any frequency within a suitable range , as well as for measurement of skin or tissue properties . such a system can be used for treating any of a variety of skin disorders , including hirsuitism , telangiectasia , pigmented lesions and the like . it will be apparent to those skilled in the art that where such degrees of versatility and usage in different possible applications are not required , a simpler and less expensive system will often suffice . in addition , if a manually moveable applicator head is not required , the system can be simplified in this respect as well . in the most rudimentary example , a monofrequency unit with means for adjusting dosage driving a fixed applicator head may be adequate . referring to fig1 , in a system 10 in accordance with the invention microwave energy of a selected frequency can be generated by any one of a number of conventional devices , such as a variable frequency synthesizer 14 that covers a range from about 2 ghz to about 20 ghz . a number of other conventional microwave generators are tunable in the range of 2 . 45 ghz to 18 ghz , for example , but here a suitable combination includes the frequency synthesizer 14 and a traveling wave tube system 12 having internal power and a high power output amplifier . where operating conditions are well - defined and wide tunability is not needed , a conventional low cost source such as a magnetron may be used . the output of the traveling wave tube system 12 is gated open for selected intervals by control pulse circuits 16 , which can be set , in this example , for any interval from 10 to 1000 milliseconds . thus , the selected frequency is delivered as a pulse burst to provide from 50 w to as much as 4 kw output , the power level most often being of the order of a few hundred watts . in transmission to the operative site , the power bursts are directed through a power sensor 18 , which diverts both forward and reverse propagated energy samples to a power meter 20 . readings at the power meter 20 enable the surgeon to fine tune power , phase or frequency settings to improve impedance matching and energy efficiency . preinspection of the target site is dependent on the nature of the target . although visual inspection is sometimes alone sufficient for target area selection , as with hirsuitism , target veins at depth below the surface can often better be identified , located , and dimensioned by conventional analytical instruments , such as those using ultrasound imaging . as is described hereafter , the power , duration and frequency applied can also be adjusted in relation to the thermal relaxation characteristics of a target blood vessel , which in turn is dependent on size and location . a microwave transmission line 24 , here including a flexible rectangular waveguide or a flexible coaxial section 26 that may be manually manipulated , supplies the microwave energy through a phase shifter or other kind of tuner 27 to a hand applicator 30 shown here as positioned against a limb 32 exposed within a surgical drape 34 . the handpiece 30 , shown in greater detail in fig2 and 3 , is essentially a rectangular waveguide device having a stepped or other impedance matching section 36 coupled to the flexible coaxial line 26 . the handpiece 30 includes a converging tapered body 38 having an open aperture end 40 serving as the wave launching terminus . internal to the tapered waveguide section 38 is a dielectric insert 44 here formed of two high dielectric ( k = 16 ) tapered strips 46 , 47 held in place between low dielectric constant ( k = 2 . 5 ) spacers 48 of a virtually microwave transparent material such as “ rexolite ”. this configuration of dielectrics , as seen in fig3 , spreads the electric field distribution toward the sidewalls , enlarging the target area that is effectively acted upon by the wave energy and eliminating any hot spot tendency within the target area . in addition , the dielectric insert 44 provides a better impedance match to the skin , reducing reflective losses , which can further be minimized by adjustments at the tuner 27 . the dielectric 44 also reduces the cross - sectional area and size of the waveguide , thereby making the handpiece 30 easier to handle . in addition , the internal taper matches the waveguide impedance to the different impedance of the dielectric loaded section , so as to minimize reflection . the flexible coaxial line 26 allows a surgeon to move the applicator 30 to place its open end manually wherever desired on the body surface 32 . at the frequency range of 12 - 18 ghz , a standard wr 62 waveguide section with 0 . 622 ″× 0 . 311 ″ orthogonal dimensions can be employed at the output end of the impedance matching section 36 . the tapered section 38 , loaded by the dielectric 44 in this example , reduces the waveguide dimension to 0 . 250 ″× 0 . 150 ″ at the output terminal face 40 . the end face 40 , however , is set off from the limb or other body surface 32 against which it is juxtaposed by an encompassing and intervening spacer element 54 , best seen in fig2 and 3 . the spacer element 54 includes an interior shoulder 56 extending around the periphery of the end 40 of the tapered section 38 , defining a standoff volume of a height of about 0 . 020 ″ ( 0 . 5 mm ). a coolant can thus be injected via a side conduit 58 from a pressurized coolant gas source 60 ( fig1 ), via a coupling conduit 62 extending through a solenoid controlled valve 64 . the pulse control 16 opens the valve 64 in timed relation to the microwave pulse to be delivered from the traveling wave tube system 12 . this timing relation can be controlled , so that the target skin area can be precooled prior to delivery of the microwave pulse , cooled concurrently with the delivery or cooled after the start of the delivery of the microwave pulse . furthermore , a temperature sensor 68 , shown only generally in fig1 , may be disposed within the standoff volume , in contact with the skin or otherwise , to sense the lowering of temperature at the target surface . in this example , the coolant is a pressured gas , such as 1 , 1 , 1 , 2 tetrafluoroethane , held under high pressure in liquefied or gaseous phase . when injected by actuation of the valve 64 , the gas expands vigorously within the standoff volume , rapidly lowering the temperature because of the expansion effect . since the boiling point of the tetrafluoroethane is approximately − 26 ° c . at 1 atm , it is extremely effective in extracting thermal energy from the target area , even for the short bursts of the order of a fraction of a second that are involved in the present procedure . the temperature sensor 58 may be a luxtron fiber optic device for measuring temperature , or it may be a thermistor which is coupled in a circuit that triggers the microwave pulse when the coolant has adequately lowered the temperature at the skin surface or in the standoff volume . other coolants , including air , can alternatively be used to reduce the skin surface temperature within the standoff volume during the procedure . other alternative approaches may be utilized to minimize discomfort and , separately or additionally , provide improved efficiency . a compound that is complementary to the delivery of the microwave energy , in the sense of neither being reflective or absorptive , and therefore not appreciably heated , can be placed on the skin prior to microwave pulse application . for example , a topical anesthetic having short term effectivity may be all that is needed to reduce the discomfort of some patients to an acceptable level . other patients may require no coolant or topical anesthetic whatsoever . another alternative is to employ a surface gel or other substance that improves impedance matching between the microwave pulse launching device and the surface tissues . the microwave delivery system provided by the applicator 30 delivers microwave energy over an advantageously broad field distribution into a subcutaneous surface area as best understood by reference to fig3 . the dielectric loading introduced by the spaced apart dielectric elements 46 , 47 , which diverge toward the output end as the sidewalls converge in the tapered section 38 , alters the normal horizontal electric field distribution from its normal half sine wave characteristic so that there is substantial field strength at the two sidewalls and no high central energy peak . a single , appropriately shaped , dielectric element can be used to modify the field distribution to like effect . by thus spreading the energy across the target area , there is both elimination of localized energy concentrations ( and therefore localized heating ) and a larger effective treatment area . as seen in the graphical portion of fig3 , in the solid line , the calculated electric field at the skin surface when the outlet end 40 of the microwave launcher is 0 . 5 mm off the surface , is more than twice that at the edges . this differential is reduced when the field distribution is modeled at a depth of 0 . 5 mm below the skin surface . in both instances , there is a degree of dispersion outside the perimeter of the applicator face 40 because of the setoff spacing , but this aids in equalizing the power distribution and poses no radiation danger . in accordance with the present invention , advantage is taken of the results of an analysis of the interaction of microwaves with biological tissues at different frequencies . the complex permittivity ∈* of any given matter , including biological matter , in a steady state field is conventionally analyzed using the following equation : in which ∈ 0 is the dielectric constant of free space and the real component , ∈′, is the dielectric constant , while the imaginary component , ∈″ is the loss factor . as seen in fig7 , the loss factor (∈″) of blood , in the range of 2 to 20 ghz , shown by tests to be substantially higher than that of skin tissue . further analysis has ascertained that by considering both relative and absolute factors , the most advantageous conditions exist at about 14 ghz . from published work , the dielectric constant of skin is known to be about 22 at 10 ghz and to decrease with increasing frequency to a value of 12 at 18 ghz . the loss factor for skin reaches a peak of 18 at 9 ghz and decreases with increasing frequency to a value of 12 at 14 ghz . the loss factor ∈″ for skin is approximately one - half that for blood in the frequency range between 14 ghz and 20 ghz , and above 10 ghz the loss factor for blood increases somewhat more than for skin , as seen in fig7 . therefore , the heat generated per unit volume in blood and to some extent in differentiable cellular structures other than skin , can be expected to be twice that of skin . consequently , differential heating results when microwave energy penetrates subcutaneous regions . because these subcutaneous regions are of depths up to 5 mm , they are directly within the range of interest that includes hair follicles and roots , telangiectasia , pigmented lesions , and other histological features that are visible through the epidermis and / or dermis , or actually protrude at the skin . the structure of skin is somewhat idealistically and simplistically depicted in fig4 , in order to show the physical relation and relative proportions ( although not to scale ) between the epidermis and dermis layers that lie above subcutaneous tissue , and to further represent histological features of interest in the structure . sweat glands , nerve endings , corpuscular structures and sebaceous glands are not included for clarity . the hair shafts , most deeply embedded at their roots at 4 to 5 mm depth in the dermis , extend outwardly through the dermis and the relatively more robust epidermal layer . relatively large arteries and veins branch into the arteriole and venule vessels which feed and derive blood , respectively , as the smallest capillaries that normally are invisible from the skin surface , and that form the termini of the blood paths . when these capillaries , either or both arterioles and venules , become engorged for some reason , as in the telangiectasia condition , they form the lateral and visible pattern , known collectively as spider veins , at a depth of 0 . 1 to 1 . 0 mm below the surface of the epidermis . typically of the order of 0 . 2 mm in diameter , the spider veins can actually sometimes protrude at the surface , and be larger in diameter as well . reticular or feeder veins can lie as much as 5 mm in depth below the surface , and are substantially larger , of the order of 1 . 0 to 2 . 0 mm in diameter , being large enough to be identified by a non - invasive inspection technique , such as imaging with ultrasound . the reticular or feeder veins sometimes create the overpressure condition causing engorgement of the spider veins . fig5 shows further details , again somewhat idealized , of an enlarged hair shaft , extending outwardly from a root into the growing cellular structure of the follicle and the follicle casing that transforms into the hair shaft body that passes through the epidermis . the hair follicle is nourished by at least one artery that feeds the papillae structure at the root and is encompassed in a crown of associated matrix cells . attack on the cellular follicle structure or on the papillae or the arterioles or venules to and from the papillae can result in permanent destruction of the hair shaft . with these considerations in mind , appreciation of the operation of the system of fig1 can more readily be gained . the surgeon can use a suitable frequency for a chosen histological feature within the range of the frequency synthesizer 14 . it is assumed here that the frequency chosen is about 14 ghz . the traveling wave tube system 12 is set to generate approximately 100 to 300 watts , the control pulse circuits 16 being set to open the solenoid valve 64 prior to getting a short pulse from the microwave system 12 . it has been found that a 100 millisecond pulse is satisfactory for both efficacy and safety , although other durations can be used with wattage adjustments to compensate . the output from the traveling wave tube system 12 is directed through the power sensor 18 , the transmission line 24 , the flexible section 26 , through the tuner 27 and to the applicator 30 . if the operator desires , short test pulses of low amplitude can first be sent to obtain readings of the reflected power at the power meter 20 , and fine tuning adjustments can be made at the tuner 27 , in a conventional manner . in addition , the operator can use ultrasound or another non - invasive diagnostic system to analyze the substructure to identify the position of target features , such as reticular veins and arteries , both as to size and location . the procedure initially to be described , however , pertains to depilation , so that the target area is not only readily visible , but is also substantially uniform in depth and structure , as per fig5 . when the control pulse circuits 16 operate , they first provide a control impulse to open the solenoid valve 64 , in this example , and then turn on the traveling wave tube system 12 for the selected interval . because the valve requires a few milliseconds ( e . g ., 20 to 35 ) to operate and a few milliseconds are also needed for the pressurized coolant from the source 60 to pass through the outer conduit 62 and the side conduit 58 in the spacer 54 , it is preferred to delay the microwave pulse until cooling has actually begun or is contemporaneously begun . alternatively , as previously noted , a temperature sensor 68 that detects a temperature drop at the skin surface may be used to either trigger the microwave pulse or to preclude its operation until after the coolant has become effective . for depilation , pulses in the range of 10 to 20 joules in terms of total work output have been shown to effect permanent depilation without significant discomfort or significant adverse side effects . tests were run using the dielectric loaded applicator 30 having a 0 . 250 ″× 0 . 150 ″ output area ( 5 mm × 3 mm , or 15 mm 2 ), and employing a pulse duration of 100 milliseconds in all instances . a substantial number of experiments were run on test rabbits with this applicator , varying only the power applied so as to change the total energy in joules . the results were examined by a pathologist and the accompanying tables 1 and 2 , appended following the specification , show the results of his examination . the system of fig1 was also employed in a number of tests on rabbits to determine the changes occurring in veins and arteries under different pathological changes , and side effects on tissues and vessels with a protocol using cooling as well as no cooling to determine if pigmentation has an effect are shown in appended table 3 . these tests showed no significant difference in pigmentation versus non - pigmentation , indicating that coloration , and / or the presence of melanin , is not a significant factor in absorption of microwave energy . a different protocol was followed in amassing results shown in appended table 4 , which represents an analysis by a pathologist blinded to the dosages used . cooling was not used in this example . these results with test rabbits show that pigmentation is not a significant factor and that at 16 joules dosage and above , there is effective occlusion of target veins and arteries with minimal changes or only mild induration of tissues . the indication of dermal fibrosis again is not indicative of scar development . pathological examination of these animal studies consistently demonstrated destruction of hair follicles over a wide range of microwave energy levels . the destruction extended to the base of the follicle , which is significant to permanent hair removal . the amount of hair destruction within the target area varies in accordance with the total amount of energy , but destruction is substantially complete at 14 joules and higher . furthermore , until the energy delivered is in excess of 20 joules , the appearance of the skin is normal in all cases and the epidermis is histologically intact . minor indications of dermal fibrosis are not indicative of clinical scar formation . minor vascular changes , such as intimal fibrosis of small arteries , constitute neither damaging nor permanent conditions . consequently , a dosage in the range of 14 to 20 joules is found both to be effective and to be free of deleterious side effects . the effects of delivery of microwave energy , with surface cooling , are illustrated graphically in fig8 , which indicates temperature changes at both the surface of animal skin tissue ( 0 . 75 mm thick ) and 1 . 5 mm below the surface , in water , under conditions of delivery of up to 12 joules total energy level over 100 milliseconds duration , accompanied by cooling using expanded tetrafluorethane gas . as shown , the baseline temperature for the test animal skin is approximately 32 ° c ., and that for the body at a depth of 1 . 5 mm is approximately 37 ° c . applying the microwave energy with cooling , the skin surface temperature rose very slightly , but was essentially unchanged . beneath the skin surface , however , the temperature rise at 1 . 5 mm depth was at a substantially higher rate , reaching approximately 60 ° c . at 100 milliseconds . higher temperatures would of course be reached with the application of higher energy levels . it is posited that even such a temperature is sufficient to cause cellular degradation of the hair follicles near the root , and it may well also thermocoagulate blood in the feeder artery , in the papillae at the hair root , or in the cell matrix surrounding the papillae . although the hair follicles are not conductive , they may be particularly susceptible to the impinging microwave energy because they are thin dielectric elements which can cause energy concentration and therefore greater heating . whether one or more effects are observable , permanent destruction has been shown by pathological examination , as in the annexed tables . the microwave energy does not significantly penetrate beyond the depth of the targeted histological features because of attenuation , the limitation on total energy delivered and the lower loss factor in tissue . where the histological defects are benign vascular lesions , as with the telangiectasia condition , different tests and operating conditions may be employed , as shown in the steps of fig6 , to which reference is now made . while spider veins can cover a substantial area , and visual targeting may be sufficient , it is often desirable to analyze the target area in greater detail . thus , ultrasound examination may be utilized to identify and estimate the size of reticular veins feeding a substantial area of spider veins , as an optional first step 80 , which can precede marking of the target surface 82 in any appropriate way . again , the dielectric constant , skin impedance or other characteristics may be tested in a preliminary step 84 , prior to choosing operative frequency in step 86 . fine tuning , phase adjustment or another impedance matching option 88 may be employed to reduce reflective losses and increase efficiency . given the size and location of the target vascular feature , thereafter , the power level and pulse duration may be selected in a step 90 . the pulse duration is a significant parameter in relation to the vessel diameter , since the smaller the vessel diameter , the shorter is the thermal relaxation time . even though the loss factor of blood is higher than that of the tissue , dissipation of heat to surrounding tissue is much faster with a small blood vessel and consequently shorter term heating is needed . as seen in fig9 , thermal relaxation time increases monotonically with vessel diameter , and thus a longer duration pulse is needed , perhaps at the same or a greater power , if the vessel diameter is of a larger size . given the power level and pulse duration , the operator can select one of the cooling options , which also includes no cooling whatsoever , in step 92 . typical anesthetics or other anesthetics may be employed at the same time , as shown by optional step 94 . consequently , when the microwave pulse is delivered , the subcutaneous target is heated to the range of 55 ° c . to 70 ° c ., sufficient to thrombose the vascular structure and terminate flow permanently . the specific nature contributing factors to disappearance of the vessels with time may be one or more factors , including thermocoagulation of the blood itself , heating of the blood to a level which causes thrombosis of the vessel or some other effect . the net result , however , is that a fibrous structure forms in the vessel which clogs and terminates flow , so that the resultant fibrous structure is reabsorbed with time , as new capillary flow paths are found . in any event , heating in the 55 ° c . to 70 ° c . is sufficient to effect ( step 96 ) the permanent pathological change that is desired ( step 98 ). an alternative applicator that covers a larger area and is employed with a peelable indicia label as shown in fig1 . the standard wr 62 waveguide for transmission of microwave energy at 14 ghz has , as previously mentioned , interior dimensions of 0 . 622 ″× 0 . 311 ″. an applicator 100 employing such a waveguide section 101 is used directly , without internal dielectric loading , to cover a substantially larger target area while employing air cooling . the waveguide section 101 , coupled via a flexible waveguide and an impedance matching transition ( not shown ), if necessary , to a microwave feed system 102 has side wall ports 104 coupled to an external coolant source 105 which may deliver coolant through a control device 106 triggered , in relation to the microwave pulse , as previously described . under some circumstances , when air is used as the coolant , it may simply be delivered continuously into the waveguide , the end of which can be blocked off by a microwave transmission window so that only the launching end and the skin surface are cooled . for use in a depilation procedure , the skin surface of a patient to be treated is covered with a sheet 108 having numbered guide indicia 109 for marking successive applicator 100 positions . these positions overlap because of the fact that the energy concentration is in the central region of the waveguide 101 , at the normal maximum amplitude of the electric field in the te 10 mode . the peel off label sheet 108 is covered on its skin - adhering side by a separable adhesive . consequently , when the applicator 100 is moved between successive overlapping index positions marked 1 , 1 , 2 , 2 etc . at the side and corner of each position , the internal areas that are pathologically affected within each location are essentially contiguous , until the entire applicator 100 has been moved through all positions on the sheet 108 , with dosages applied to all of the areas . hair follicles having been destroyed in those areas , the procedure is terminated and the sheet 108 is peeled off , with the destroyed hair follicles and shafts adhering to it . with the arrangement of fig1 , a longer microwave pulse duration or more wattage is needed for increasing the number of joules because of the broader beam distribution , which means that , heating is at a slower rate ( e . g ., in the approximate proportion of 0 . 7 ° c . rise in skin temperature per joule for the large applicator versus 2 . 4 ° c . per joule for the dielectric filled smaller applicator ). the skin temperature rise was reduced by a factor of 2 when using air at a temperature of between 0 ° c . and − 5 ° c . it should be noted , furthermore , that a standard open rectangular waveguide can be loaded with dielectric elements in a manner which enables size to be reduced without restricting coolant flow . another alternative that may be used , but is not shown in the figures , relates to a modification of the spacer element that is employed in the example of fig2 and 3 . one can configure the spacer element with two alternative but adjacent positions for the applicator open ( emitter ) end , and arrange the applicator so that the emitter end can be shifted between the two positions . in a first or reserve position of the applicator , the target surface can be viewed through the spacer element , and positional adjustments can be made . this part of the spacer element is then used as a frame for visualizing the operative target on the skin surface when the applicator is in the reserve position . as soon as the target area is properly framed , the applicator is simply shifted from the reserve position to the operative position , in proper alignment with the target area , and the procedure can begin . a different approach to a useful applicator is shown in fig1 , to which reference is now made . this also illustrates a different means for cooling the skin surface , as well as for viewing the target area . in this example , the applicator 120 comprises an open - ended wave propagation segment 122 fed via a transition section 124 from a coaxial line 126 . the unit may be physically manipulated by an attached handle 128 . the open end of the waveguide 122 is filled by a dielectric element 130 which is not only of suitable electrical dielectric properties but a good heat conductor as well , such as boron nitride or beryllium oxide . the dielectric insert 130 extends beyond the open end of the waveguide , into contact with a skin surface that is to be exposed to microwave radiation . the interior end of the dielectric 130 is urged in the direction toward the skin surface by a non - conductive , non - absorptive microwave leaf spring 134 of selected force and compliance . thus , the dielectric insert 130 presses on the skin surface with a yieldable force , selected to assure that contact is maintained but that any protruding veins or arteries are not closed simply by the force of the applicator 120 . this applicator 120 and dielectric insert 130 are externally cooled by an encompassing sleeve 136 through which coolant is passed via internal conduits 137 , 138 that communicate with an external supply ( not shown ) via external conduits 141 , 142 . consequently , heat is extracted from the surface of the skin via the contacting dielectric 130 itself . in addition , a target mark placed on the skin surface by the surgeon may be viewed by a system including a fiber optic line 145 that extends through the dielectric 130 and leads via a flexible fiber optic line 147 to an image viewing system 149 . in use , this applicator 120 of fig1 covers a substantial chosen area , with the viewing and cooling features that simplify placement and minimize discomfort . the movable dielectric insert 130 can be a replaceable element , with different shapes of dielectrics being submitted where different conditions apply . it will be appreciated that other expedients may be utilized for shaping the microwave beam , including lens and diffuser systems . although a number of forms and modifications in accordance with the invention have been described , it will be appreciated that the invention is not limited thereto , but encompasses all forms and expedients in accordance with the appended claims .
a system and method for treating subcutaneous histological features without affecting adjacent tissues adversely employs microwave energy of selected power , frequency and duration to penetrate subcutaneous tissue and heat target areas with optimum doses to permanently affect the undesirable features . the frequency chosen preferentially interacts with the target as opposed to adjacent tissue , and the microwave energy is delivered as a short pulse causing minimal discomfort and side effects . by distributing microwave energy at the skin over an area and adjusting power and frequency , different conditions , such as hirsuitism and telangiectasia , can be effectively treated .