as will be described in detail hereinafter , an aspect of the present disclosure envisages providing a microelectromechanical gyroscope having an arrangement of the sensing masses such as to enable an increase in the sensitivity of the sensor and in general an improvement of its electrical characteristics . as is shown in fig4 , where the same reference numbers are used for indicating elements similar to others already described with reference to fig1 , the microelectromechanical gyroscope , here designated by 30 , differs from the gyroscope 1 of fig1 substantially on account of a different arrangement of the first sensing masses , here designated by 16 a ′- 16 d ′, and of the second sensing masses , here designated by 25 a ′, 25 b ′. in greater detail , the first sensing masses 16 a ′, 16 b ′ of the first pair are aligned in a first diametric direction x 1 , inclined with respect to the first horizontal axis x of the die 2 by an angle of inclination α ( considered in a counterclockwise direction ), the value of which is preferably 45 °. likewise , the first sensing masses 16 c ′, 16 d ′ of the second pair are aligned in a second diametric direction x 2 , substantially orthogonal to the first diametric direction x 1 , and inclined with respect to the first horizontal axis x by the same angle of inclination α ( considered in this case in an opposite direction , namely clockwise ). the first sensing masses 16 a ′- 16 d ′ are consequently aligned in respective diametric directions , which are inclined with respect to the pitch and roll axes , about which the pitch angular velocity { right arrow over ( ω )} x and the roll angular velocity { right arrow over ( ω )} y are applied , and moreover inclined with respect to the sides of the die 2 ( and to the horizontal axes x , y ). in addition , the first sensing masses 16 a ′, 16 b ′ of the first pair are symmetrical to corresponding sensing masses 16 d ′, 16 c ′ of the second pair , with respect to the axis of symmetry of the die pads 2 d ( coinciding with the second horizontal axis y ). the second sensing masses 25 a ′, 25 b ′ are arranged in the available space left free by the first sensing masses 16 a ′- 16 d ′, and are , for example , aligned along the second horizontal axis y ( as illustrated in fig4 ). it may thus be noted that the arrangement of the first and second sensing masses in fig4 derives , as compared to the arrangement of the same masses of fig1 , from a counterclockwise rotation through the angle of inclination α about the center o . the present applicant has found that the aforesaid arrangement of the first and second sensing masses 16 a ′- 16 d ′, 25 a ′, and 25 b ′ makes it possible to achieve a series of advantages , amongst which a simplified connection of the corresponding first and second sensing electrodes 22 , 23 towards the die pads 2 d . in particular , a first processing channel in the electronic read interface and corresponding electrical connections to the connection pads 2 d are associated to the first pair of first sensing masses 16 a ′, 16 b ′, whilst associated to the second pair of first sensing masses 16 c ′, 16 d ′ are , in the same electronic read interface , a second and distinct processing channel , and corresponding electrical connections to the respective connection pads 2 d . the present applicant has found that in the arrangement of a known type shown in fig1 , the position of the first sensing masses 16 a - 16 d with respect to the connection pads 2 d of the die 2 shows a marked lack of uniformity ( as do the corresponding electrical connections to the same connection pads 2 d ). in fact , the two pairs of first sensing masses 16 a - 16 d are mutually positioned in an asymmetrical way with respect to the axis of symmetry of the connection pads 2 d , thus calling for a different design of the electrical connections for the two processing channels . consequently , the reading performance referred to the two axes of detection ( of pitch and roll ) may be different , and possibly must be compensated for by the electronic read interface ( which is consequently more complex ). instead , the arrangement described in fig4 for the first sensing masses 16 a ′- 16 d ′ with respect to the connection pads 2 d makes it possible to obtain a substantial symmetry of the electrical connections to the connection pads 2 d for the two processing channels ( the two pairs of first sensing masses are in fact set in an altogether symmetrical way with respect to the axis of symmetry of the connection pads 2 d ). the symmetry of the electrical connections enables considerable advantages to be obtained in terms of uniformity in the electrical characteristics ( for example , in terms of active and parasitic capacitances , or leakage currents ) and robustness to the spread of the parameters resulting from the manufacturing process . advantageously , the arrangement described enables an increase of the symmetry also of the electrical connections referred to the second sensing masses 25 a ′, 25 b ′, thus leading to an increase of uniformity in the electrical characteristics of the corresponding read electronics . in particular , the arrangement of the second sensing masses 25 a ′, 25 b ′ guarantees a substantial symmetry of the overall structure with respect to the axis of symmetry of the connection pads 2 d , thus further simplifying the design of the electrical connections . fig5 shows a variant embodiment of the gyroscope 30 , which differs from the one shown in fig4 in so far as the second sensing masses 25 a ′, 25 b ′ are aligned along the first horizontal axis x , instead of along the second horizontal axis y . also in this case , the same considerations made previously still apply . in particular , this configuration intuitively enables a further increase in the symmetry of the detection structure with respect to the axis of symmetry of the die pads 2 d . the present applicant has found that the aforesaid arrangement of the first and second sensing masses 16 a ′- 16 d ′, 25 a ′, and 25 b ′ also optimizes exploitation of the space available in the gyroscope for detection of the angular velocity . the area available for providing the detection structures , coinciding with the open region 2 c defined by the frame 2 b of the die 2 , in fact usually has a square shape ( as is shown in fig4 and in fig6 ) or a rectangular shape . the arrangement of the first sensing masses 16 a ′- 16 d ′ in directions inclined with respect to the sides of the frame 2 b and to the horizontal axes x , y enables increase of the dimensions and maximization of the sensitivity of the first sensing masses , exploiting for detection the areas at a greater distance from the axis of rotation of actuation . in greater detail , and as is shown in fig6 , which represents in a simplified way just the area available ( open region 2 c ) of the gyroscope 30 and a first sensing mass ( for example , the first sensing mass 16 a ′), the conformation of the first sensing masses 16 a ′- 16 d ′ can in this case be modified so as to improve exploitation of the space available in a radial direction , until the internal edges of the frame 2 b are approached . in a way not illustrated , also the conformation of the driving mass 3 , within the overall dimensions of which the sensing masses are housed , is in this case modified . in particular , represented with a solid line is a variant embodiment of the first sensing mass 16 a ′, having in this case a generally rhomboidal shape extending towards an internal edge of the frame 2 b and its center of gravity g ′ located at an arm b c ′ from the first elastic supporting elements 20 . in fig6 , illustrated with a dashed line , purely to facilitate a comparison between the different solutions , is a first sensing mass of a traditional type ( for example , the first sensing mass 16 b of fig1 ), having the shape , described previously , of a radial sector . the first sensing mass 16 b of a traditional type has its center of gravity g located at an arm b c from the respective first elastic supporting elements 20 . both of the first sensing masses illustrated are located at one and the same radial distance d between the respective first elastic supporting elements 20 and the center o . this comparison highlights the fact that the arm b c of the traditional sensing mass has a value visibly smaller than that of the arm b c ′ that can be obtained in the new configuration . in particular , the increase of the distance of the center of gravity g ′ of the first sensing masses 16 a ′- 16 d ′ from the center o enables an increase in the driving velocity { right arrow over ( ν )} a felt by the same first sensing masses ( given the same angle of rotation of the driving mass 3 ), and hence an increase in the coriolis force f c ′, given that this force is directly proportional to the driving velocity { right arrow over ( ν )} a . in addition , since the coriolis force f c ′ is applied at a greater arm b c ′, the value of the resulting twisting moment increases . in addition , this configuration allows to have available a greater surface for the sensing electrodes 22 , 23 . in general , it is thus clear that this configuration enables , with appropriate design choices , a considerable increase in the sensitivity of detection . the present applicant has also found that the aforesaid arrangement of the first and second sensing masses 16 a ′- 16 d ′, 25 a ′, and 25 b ′ makes it possible to obtain , using an appropriate configuration of the electronic read interface , a further increase in the sensitivity of the gyroscope 30 . in detail , the gyroscope 30 , shown in fig4 and 5 , has the peculiarity of having the axes of detection in the plane of the sensor xy ( coinciding with the first and second diametric directions x 1 , x 2 of alignment of the first sensing masses 16 a ′- 16 d ′) inclined by the angle α with respect to the horizontal axes x and y about which the pitch angular velocity { right arrow over ( ω )} x and the roll angular velocity { right arrow over ( ω )} y act . instead of envisaging assembly of the die 2 rotated by a corresponding angle α at the level of package or board , which would evidently make it possible to re - orient the axes of detection according to the original directions of pitch and roll ( i . e ., the horizontal axes x and y ), a further aspect of the present disclosure envisages to suitably combine at the electronic read interface level the detection signals coming from the first sensing masses 16 a ′- 16 d ′. in particular , the detection signals are combined so as to re - obtain , starting from the capacitive variations associated to the displacements of the first sensing masses 16 a ′- 16 d ′, voltage outputs corresponding to the original pitch and roll directions ( i . e ., to the horizontal axes x and y ). in the case where the angular velocity to be detected about the first horizontal axis x or the second horizontal axis y , a unit value is considered for simplicity : and each pair of first sensing masses 16 a ′- 16 d ′ has a unit sensitivity s : intuitively , in the case of a traditional configuration ( for example , of the type illustrated in fig1 , having first sensing masses 16 a - 16 d aligned along the horizontal axes x , y ), the following voltage values would be obtained at an output from the electronic read interface : where v out , x ( is the output voltage corresponding to the first pair of first sensing masses 16 a , 16 b aligned along the first horizontal axis x , and v out , y is the output voltage corresponding to the second pair of first sensing masses 16 c , 16 d aligned along the second horizontal axis y ( in the traditional solution ). in particular , as described previously , an angular velocity ( of pitch or roll ) about one of the horizontal axes x , y would determine a capacitive unbalancing of a single pair of first sensing masses 16 a - 16 d ( in particular the pair aligned about the same horizontal axis ). instead , in the new configuration illustrated in fig4 or in fig5 , an angular velocity ( of pitch or roll ) about one of the horizontal axes x , y determines a capacitive unbalancing of both of the pairs of first sensing masses 16 a ′, 16 b ′ and 16 c ′, 16 d ′, in so far as they are sensitive to the components of the angular velocities of pitch and roll along the diametric directions x 1 and x 2 , and these components have a non - zero value for both of the pairs . given the same geometry and distance from the center o of the first sensing masses 16 a ′- 16 d ′, in this case the following total output voltages for the horizontal axes x , y are obtained : where v out , x1 and v out , x2 are the output voltages corresponding to the first pair and , respectively , to the second pair of first sensing masses 16 a ′- 16 d ′, aligned , respectively , in the first and second diametric directions x 1 , x 2 . consequently , although the capacitive unbalancing of the single first sensing masses referred to a given angular velocity is smaller by a factor 1 /√{ square root over ( 2 )} with respect to the corresponding unbalancing in a traditional configuration , it is possible to sum ( via a purposely configured read interface ) the contributions of all four of the first sensing masses referred to the same angular velocity , and obtain a global increase in the sensitivity of the gyroscope 30 by a factor √{ square root over ( 2 )}. fig7 illustrates an electronic device 40 , which comprises the microelectromechanical gyroscope 30 described previously . the electronic device 40 can advantageously be used in a plurality of electronic systems , for example , in inertial navigation systems , in automotive systems , or in systems of a portable type , such as , for example : a pda ( personal digital assistant ); a portable computer ; a cell phone ; a digital audio player ; a photographic camera or a camcorder ; or further systems capable of processing , storing , transmitting , and receiving signals and information . the electronic device 40 further comprises : a driving circuit 41 , operatively coupled to the driving assembly 4 for imparting the rotary driving movement to the driving mass 3 , and supplying biasing signals to the microelectromechanical structures ; a read circuit 42 , operatively coupled to the sensing electrodes 22 , 23 of the first and second sensing masses , for detecting the amount of displacement of the same sensing masses and hence determining the angular velocities acting on the structure ; and an electronic control unit 44 , for example , of a microprocessor type , connected to the read circuit 42 , and designed to supervise the general operation of the electronic device 40 , for example , on the basis of the angular velocities detected and determined . in particular , the read circuit 42 includes the aforesaid electronic read interface , designed to appropriately combine the output signals corresponding to the individual first sensing masses , in order to increase the sensitivity of detection , as described previously . the advantages of the microelectromechanical gyroscope provided according to the present disclosure are clear from the foregoing description . in any case , it is once again emphasized that the configuration of the sensing masses makes it possible to optimize exploitation of the area available for detection , increase the sensitivity of the sensor , and improve uniformity of the electrical characteristics and the robustness of the system to disturbance . more in general , this configuration allows improving the characteristics and the electrical performance of the microelectromechanical gyroscope . finally , it is clear that modifications and variations can be made to what has been described and illustrated herein , without thereby departing from the scope of the present disclosure . in particular , it is evident that the new configuration of the first sensing masses can advantageously be provided for a gyroscope that is only biaxial , i . e ., not sensitive to yaw angular velocity ( and hence without the second sensing masses 25 a ′, 25 b ′). for specific design requirements , the value of the angle α may differ from the value described , and be , for example , comprised between 40 ° and 50 °. the angles of inclination of the two pairs of first sensing masses 16 a ′- 16 d ′ with respect to the first horizontal axis x may also not be the same , the two pairs of first sensing masses having in any case opposite inclination with respect to the first horizontal axis x , but in this case no longer be symmetrical with respect to the second horizontal axis y . in addition , the two diametric directions x 1 and x 2 may not be orthogonal to one another . in addition , the die pads 2 d can extend in a different direction , for example , along the second horizontal axis y . in a per - se known manner , the displacement of the sensing masses can be determined with a technique different from the capacitive one , for example , by detection of a magnetic force . in addition , the twisting moment for causing oscillation of the driving mass with rotary movement can be generated in a different way , for example , by means of parallel - plate electrodes , or else by magnetic actuation . more in general , it is evident that the configuration of some structural elements of the gyroscope may be different . for example , the driving mass 3 may have a shape different from the circular one , such as a generally closed polygonal shape , as likewise the shape of the frame 2 b of the die 2 can be different . alternatively , it is possible to envisage a different arrangement of the first elastic anchorage elements of the driving mass 3 ( which must be in any case able to perform decoupling of the driving mass from the motion of detection ), or of the second elastic supporting elements 28 ( which must be in any case such as to enable the radial movement of the sensing masses of the second type ). in addition , a different configuration of the sensing electrodes associated to the sensing masses of the first and second types can be envisaged . the various embodiments described above can be combined to provide further embodiments . all of the u . s . patents , u . s . patent application publications , u . s . patent applications , foreign patents , foreign patent applications and non - patent publications referred to in this specification and / or listed in the application data sheet are incorporated herein by reference , in their entirety . aspects of the embodiments can be modified , if necessary to employ concepts of the various patents , applications and publications to provide yet further embodiments . these and other changes can be made to the embodiments in light of the above - detailed description . in general , in the following claims , the terms used should not be construed to limit the claims to the specific embodiments disclosed in the specification and the claims , but should be construed to include all possible embodiments along with the full scope of equivalents to which such claims are entitled . accordingly , the claims are not limited by the disclosure .