the preferred embodiments of this invention are tamr write heads for producing high density recording on a magnetic medium . the write head , which can be a flying type or a contact type , incorporates a plasmon generator ( pg ) ( also denoted a plasmon antenna ) of novel shape and structure that is attached to the write head so that a face of the pg emerges at the abs of the writer at a position adjacent to the abs of the main magnetic pole . the pg is radiatively coupled to optical frequency electromagnetic radiation generated preferably by an optical laser and guided by an optical waveguide ( wg ) to the pg . the radiative coupling generates surface plasmon modes within the antenna whose associated electromagnetic fields ( the near fields ) impinge on a small surface area of the magnetic recording medium , generating thermal energy within that area and causing the temperature of that area to increase . the magnetic pole of the writer produces a magnetic writing field that changes the local magnetization of the medium by switching magnetic grains within the heated spot . the shape of the pg includes a region of horizontal cross - section that is tapered in the direction of the abs . this section and an additional tip section that extends to the abs of the pg , may also be flared ( tapered in vertical cross - section ) with a flare angle that can be adjusted to optimize the plasmon energy transfer to the magnetic medium . referring to fig8 a , there is shown a schematic illustration of a side view of a first embodiment of the invention showing the magnetic write pole ( 21 ), the plasmon generator ( 23 ), the adjacent optical waveguide ( 24 ) and a small stitched pole portion ( 22 ) that serves to support and mount the antenna and to assist in sending the magnetic write field to its proper location on the magnetic medium ( not shown ). the waveguide terminates behind the stitched pole . the plasmon generator ( 23 ) transmits a plasmon mode towards the medium , which would be immediately beneath the abs surface but is not shown here , and produces localized heating within the medium by the absorption of energy from the plasmon electric field . this heating reduces magnetic coercivity and anisotropy of the medium to enable an easier switching of its magnetization . once the medium returns to ambient temperature , its coercivity and anisotropy maintains the magnetization of the previously heated region in a thermally stable mode . the waveguide ( 24 ) transmits an optical mode of electromagnetic radiation that is generated by a radiation source such as a solid state optical laser ( not shown ). the radiation from the waveguide mode couples with the plasmon mode of the generator within the overlap region ( 25 ) between the waveguide and the generator . as shown in the abs view of fig8 b , the plasmon generator in this embodiment has a triangular cross - sectional shape at its abs end . the vertex ( 26 ) of the plasmon generator ( 23 ) points towards the waveguide and the magnetic write pole ( 21 ). the write pole ( 21 ), stitched pole ( 22 ) and plasmon generator ( 23 ) are fully exposed at the abs of the tamr head . the outline of the waveguide is in broken lines ( 24 ) to indicate that it is recessed behind the stitched pole ( 22 ). in this embodiment there is also a certain spacing ( 27 ) between the plasmon generator and the waveguide and stitched pole . the dimensions of the abs cross - section are a base width between approximately 0 . 1 and 0 . 5 microns and a height from base to vertex of between approximately 0 . 05 and 0 . 5 microns . referring again to fig2 b , the shape of the pg ( 23 ) shown in fig8 a is divided into three sectors . the first sector ( farthest from the abs ), s 1 , is of uniform width ( in the x - direction ) between approximately 0 . 3 - 1 . 0 microns and a length ( in the z - direction ) of between approximately 0 . 5 - 5 . 0 microns . it is this sector that couples the waveguide ( wg ) radiation into a surface plasmon ( sp ) propagating along the interface between the pg and the cladding layer of the wg . the second , tapered , sector , s 2 , is of triangular shape and length between approximately 0 . 5 and 5 . 0 microns . it is this sector that condenses the surface plasmon in the lateral direction ( z - direction ) as it propagates towards the abs . the third sector , is a straight or tapered portion , s 3 , of length between approximately 0 and 0 . 2 microns , which further delivers the energy in the highly condensed and confined surface plasmon mode to the medium placed beneath the pg . referring finally to fig8 c , there is shown a view of fig8 a from the end opposite the abs , showing the entrance end shape of the plasmon generator ( 23 ), the cross - sectional shape of the waveguide ( 24 ) and magnetic pole ( 21 ). although the abs shape of the plasmon generator in fig7 b is shown as triangular , the various shapes in fig5 are all possible . the same is true for the back - end shape in fig8 c , where the other shapes of fig4 are equally possible . referring next to fig9 a , there is shown a schematic illustration of a side view of a second embodiment of the invention . in this embodiment the dimensions of the pg are the same as in the embodiment of fig8 a - 8 c and will not be re - iterated , but the positioning of the pg and wg are different . fig9 a shows the magnetic write pole ( 21 ), the pg ( 23 ), and a small stitched pole portion ( 22 ) that serves to support and mount the antenna and to assist in sending the magnetic write field to its proper location on the magnetic medium ( not shown ). the adjacent optical waveguide ( 24 ), in this embodiment , is located adjacent to the opposite side of the plasmon generator , so the plasmon generator is between the waveguide and the write pole ( 21 ) and stitched pole ( 22 ). the distal end of the waveguide is still recessed relative to the abs of the configuration and terminates behind the stitched pole . as shown in the abs view of fig9 b , the vertex ( 26 ) of the pg ( 23 ) points towards the magnetic write pole ( 21 ). the write pole ( 21 ), stitched pole ( 22 ) and plasmon generator ( 23 ) are fully exposed at the abs of the tamr head . the outline of the waveguide is in broken lines ( 24 ) to indicate that it is recessed behind the stitched pole ( 22 ) in this illustration , but it may equally well extend to the abs . in this embodiment there is also a certain spacing ( 27 ) between the plasmon generator and the waveguide and stitched pole . referring finally to fig9 c , there is shown a view of fig9 a from the end opposite the abs , showing the entrance end shape of the plasmon generator ( 23 ), the cross - sectional shape of the waveguide ( 24 ) at the opposite side of the plasmon generator and the magnetic pole ( 21 ). although the abs shape of the plasmon generator in fig8 b is shown as triangular , the various shapes in fig5 are all possible . the same is true for the back - end shape in fig9 c , where the other shapes of fig4 are equally possible . referring to fig1 a , 10 b and 10 c there are shown schematic illustrations of a side view , an abs view and a back end view of a third embodiment of the invention that is in all its dimensions the same as the first embodiment , except that the stitched pole portion ( 22 ) has a tapered portion ( 29 ) at the end opposite its abs end . this tapered portion allows a better propagation efficiency of the surface plasmon at the surface of the plasmon generator ( 23 ) as it propagates towards the abs of the plasmon generator . as shown in the abs view of fig1 b , the vertex ( 26 ) of the plasmon generator ( 23 ) points towards the waveguide and the magnetic write pole ( 21 ). the write pole ( 21 ), stitched pole ( 22 ) and plasmon generator ( 23 ) are fully exposed at the abs of the tamr head . the outline of the waveguide is in broken lines ( 24 ) to indicate that it is recessed behind the stitched pole ( 22 ). in this embodiment there is also a certain spacing ( 27 ) between the plasmon generator and the waveguide and stitched pole . referring finally to fig1 c , there is shown a view of fig8 a from the end opposite the abs , showing the entrance end shape of the plasmon generator ( 23 ), the cross - sectional shape of the waveguide ( 24 ) and magnetic pole ( 21 ). although the abs shape of the plasmon generator in fig1 b is shown as triangular , the various shapes in fig5 are all possible . the same is true for the back - end shape in fig1 c , where the other shapes of fig4 are equally possible . as is understood by a person skilled in the art , the preferred embodiments of the present invention are illustrative of the present invention rather than being limiting of the present invention . revisions and modifications may be made to methods , processes , materials , structures , and dimensions through which is formed and used a tamr write head with a non - uniformly shaped plasmon antenna that condenses plasmon energy as it propagates towards an abs , while still providing such a tamr write head , formed and used in accord with the present invention as defined by the appended claims .