Patent Description:
Reference will be made hereinafter, without this implying any loss of generality, to a microelectromechanical mirror device, where the tiltable structure carries, on a top surface thereof, a reflecting, or mirror, surface.

In a known manner, microelectromechanical mirror devices, in particular of the vector-scanning type (the so-called vector scanning MEMS), are used in portable apparatuses, such as, for example, smartphones or tablets, for projecting images at a distance, and in three-dimensional (3D) sensing applications, for increasing the field of view (FOV) and the resolution of projection or for creating desired patterns. Thanks to the reduced dimensions, these devices allow to meet stringent requirements as regards occupation of space, in terms of area and thickness.

These microelectromechanical mirror devices generally include a mirror structure, which is made starting from a body of semiconductor material and is elastically supported above a cavity so as to be movable, for example with a movement of inclination or rotation out of a corresponding plane of main extension, for directing an incident light beam in a desired manner.

Typically, a deflection of the incident light beam along two axes is required, which can be obtained by a single microelectromechanical mirror device of a biaxial type, i.e., one in which the mirror structure is tiltable about two rotation axes.

<FIG>, which is not covered by the subject-matter of the claims, shows schematically a mirror structure <NUM>, of a vector-scanning type, which projects at a distance an incident image (or pattern of dots) <NUM> towards a screen <NUM>.

The mirror structure <NUM> can be driven so as to carry out rotations about a first rotation axis and a second rotation axis, designated by A1 and A2, respectively, in particular assuming, according to the aforesaid rotations, four different quasi-static positions so as to direct the incident light beam <NUM> onto a projection area <NUM> on the screen <NUM>. Advantageously, said projection area <NUM> is four times larger than the area defined by the incident light beam <NUM>, consequently providing a projection with a resolution that is four times higher and a field of view that is also four times larger compared to the characteristics of the aforesaid incident light beam <NUM>.

<FIG>, which is not covered by the subject-matter of the claims, shows a further use of the mirror structure <NUM>, in this case for generating on the screen <NUM> simple patterns <NUM>, for example arrows, as in the case illustrated, indications, wordings with few letters or the like, by reflection of an incident beam <NUM> generated by a laser source <NUM>. The mirror structure <NUM> can once again be driven in rotation about the first and second rotation axes A1 and A2, in this case by performing quasi-static linear movements so as to generate the desired patterns <NUM> on the screen <NUM>.

The majority of known microelectromechanical mirror devices envisage an actuation of an electrostatic or electromagnetic type for implementing rotation of the mirror structure. Electrostatic-actuation systems generally require high operating voltages, whereas electromagnetic-actuation systems in general entail high power consumption.

Solutions based on a piezoelectric actuation have therefore been proposed, in particular by means of actuators made of PZT (lead zirconate titanate), and moreover based on detection of the extent of movement of the mirror structure by piezoresistive (PZR) sensor elements. Piezoelectric-actuation mirror devices in general have the advantage of requiring actuation voltages and power-consumption levels lower than electrostatic or electromagnetic actuation devices.

For example, <CIT>, filed in the name of the present Applicant, discloses a microelectromechanical structure provided with a structure tiltable by piezoelectric actuation having improved mechanical and electrical characteristics.

The above microelectromechanical structure comprises: a fixed structure defining a cavity; a tiltable structure, which is elastically suspended in the cavity and has a main extension in a horizontal plane; a piezoelectrically-driven actuation structure which can be biased for causing a rotation of the tiltable structure about at least a first rotation axis parallel to a first horizontal axis of the horizontal plane, the actuation structure being interposed between the tiltable structure and the fixed structure. In particular, the actuation structure comprises at least a first pair of driving arms, which carry respective piezoelectric material regions and are elastically coupled to the tiltable structure on opposite sides of the first rotation axis, by respective elastic decoupling elements, which are rigid to movements out of the horizontal plane and compliant to torsion about the first rotation axis.

The aforesaid microelectromechanical mirror structure is configured to rotate about the first horizontal axis with a resonant movement in order to generate a fast horizontal scan; as described in the aforesaid document <CIT>, the tiltable structure may moreover be driven about a second horizontal axis with a linear or quasi-static movement (i.e. at a frequency much lower than the frequency of the resonant movement) so as to generate a slow vertical scan, for example of a sawtooth type.

Even though the structure described in the aforesaid document <CIT> has several advantageous features, it is not designed for use in microelectromechanical mirror devices of the vector-scanning type (the so-called Vector Scanning MEMS), where, as mentioned previously, the mirror structure is tiltable so as to assume four different quasi-static positions.

<CIT> discloses a microelectromechanical structure having a body of semiconductor material with a fixed frame internally defining a cavity; a mobile mass elastically suspended in the cavity and movable with a first resonant movement of rotation about a first rotation axis and with a second resonant movement of rotation about a second rotation axis, orthogonal to the first rotation axis; a first and a second pair of supporting elements, which extend in a cantilever fashion in the cavity, are rigidly coupled to the frame, and can be deformed by piezoelectric effect to cause rotation of the mobile mass about the first rotation axis and the second rotation axis; and a first and a second pair of elastic-coupling elements, elastically coupled between the mobile mass and the first and the second pairs of supporting elements; the first and second movements of rotation of the mobile mass are decoupled from one another and do not interfere with one another due to the elastic-coupling elements of the first and the second pairs.

<CIT> discloses a MEMS actuating device and, more specifically, provides a MEMS actuating device which comprises an actuating unit to actuate a driven unit by being connected to a connection link of the driven unit provided with at least one protruding connection link. The actuating unit comprises an actuating arm connected to cross over a protruding direction of the connection link at one side of the connection link and an actuator actuating the actuating arm. A buffer spring is provided between the connection link and the driven unit or the connection link and the actuating arm.

The aim of the present solution is to provide a microelectromechanical device with actuation of a piezoelectric type that will allow to overcome the drawbacks of the prior art.

According to the present solution, a microelectromechanical device is provided, as defined in the appended claims.

For a better understanding of the present invention preferred embodiments thereof are now described, purely by way of non-limiting example, with reference to the attached drawings, wherein:.

<FIG> is a schematic depiction of a MEMS (MicroElectroMechanical System) device <NUM>, in particular a mirror device of the vector-scanning type, according to a first embodiment of the present solution.

The microelectromechanical device <NUM> is formed in a die of semiconductor material, in particular silicon, and is provided with a tiltable structure <NUM>, which has a main extension in a horizontal plane xy and can be driven so as to rotate about a first rotation axis A1, which is parallel to a first horizontal axis x of the aforesaid horizontal plane xy, and about a second rotation axis A2, which is parallel to a second horizontal axis y of the horizontal plane xy and defines, with the first horizontal axis x, the aforesaid horizontal plane xy (in the embodiment illustrated, the sides of the die are moreover parallel to the horizontal axes x, y).

As will be discussed hereinafter, the tiltable structure <NUM> may moreover be driven so as to carry out movements along a vertical axis z, orthogonal to the horizontal plane xy.

The first rotation axis A1 represents a first median axis of symmetry for the microelectromechanical device <NUM>; and the second rotation axis A2 represents a second median axis of symmetry for the same microelectromechanical device <NUM>, which also has a central symmetry with respect to a centre O (which moreover represents the centre of the aforesaid tiltable structure <NUM>).

Basically, the microelectromechanical device <NUM> may be ideally divided into four quadrants with respect to the aforesaid centre O, having a same arrangement and configuration.

The tiltable structure <NUM> is suspended above a cavity <NUM>, obtained in the die, and has, in the embodiment illustrated, a generically circular shape in the horizontal plane xy. The tiltable structure <NUM> carries at the top a reflecting surface <NUM>' so as to define a mirror structure.

The tiltable structure <NUM> is elastically coupled to a fixed structure <NUM>, formed in the same die. In particular, the fixed structure <NUM> defines, in the horizontal plane xy, a frame <NUM>' (in the example having a substantially squared shape), which delimits and surrounds the aforesaid cavity <NUM>, and further comprises a supporting structure <NUM> (which will be described in greater detail hereinafter), which extends within the cavity <NUM> starting from the same frame <NUM>'.

The tiltable structure <NUM> is elastically supported above the cavity <NUM> and is connected, in each quadrant, to a respective lever element <NUM>, which extends, in the embodiment illustrated, in a diagonal direction, inclined at <NUM>° with respect to the first and second horizontal axes x, y, starting from an edge portion of the tiltable structure <NUM>, at a first end thereof, towards a vertex portion of the frame <NUM>', at a second end thereof. In the embodiment illustrated, the lever element <NUM> has a substantially rectangular shape in the horizontal plane xy, elongated along the aforesaid diagonal direction.

In particular, the tiltable structure <NUM> is elastically coupled to each lever element <NUM>, at its first end, by a respective elastic suspension element <NUM>, having a high rigidity in regard to movements out of the horizontal plane xy (along the orthogonal axis z, transverse to said horizontal plane xy) and furthermore configured so as to enable a relative rotation between the same tiltable structure <NUM> and the lever element <NUM>.

In detail, each of the elastic suspension elements <NUM> comprises a first portion 18a of a folded type, connected to the aforesaid edge portion of the tiltable structure <NUM>, and a second portion 18b, of a torsional type, constituted by a rectilinear element arranged along the diagonal direction and connected between the first portion 18a and the first end of the lever element <NUM>.

Each lever element <NUM>, at its second end, is furthermore elastically coupled to the aforesaid supporting structure <NUM>, in particular by respective elastic connecting elements <NUM>, of a torsional type, having a rectilinear extension substantially transverse with respect to the aforesaid diagonal direction, on opposite sides with respect to the lever element <NUM>, to define a lever rotation axis L for the lever element <NUM>.

As will be discussed hereinafter, the lever element <NUM> is configured to rotate about the lever rotation axis L, so that its first end (coupled to the tiltable structure <NUM>) moves upwards along the vertical axis z (and consequently its second end moves downwards) or downwards (and consequently its second end moves upwards). In a corresponding manner, the tiltable structure <NUM> moves upwards or downwards at its edge portion coupled to the aforesaid first end of the lever rotation element <NUM>.

In greater detail, the aforesaid supporting structure <NUM> comprises: central arms 15a, which extend starting from the frame <NUM>' towards the tiltable structure <NUM>, in the embodiment described, along the first rotation axis A1 or the second rotation axis A2, at the centre with respect to the cavity <NUM>, terminating at a distance from the same tiltable structure <NUM>; and connecting arms 15b, having a first end elastically coupled to a respective lever element <NUM> by a respective elastic connecting element <NUM> and a second end fixed with respect to a respective central arm 15a, to which it is joined at the corresponding first rotation axis A1 or second rotation axis A2.

Consequently, in each quadrant of the microelectromechanical (MEMS) device <NUM>, two connecting arms 15b are present, extending on opposite sides with respect to the corresponding lever element <NUM>, towards a respective central arm 15a, which extends along the first, respectively, the second rotation axis A1, A2.

The microelectromechanical device <NUM> further comprises an actuation structure <NUM>, which is elastically coupled to the lever elements <NUM> and is configured to cause the movement of the tiltable structure <NUM>, namely its rotation about the first rotation axis A1 and the second rotation axis A2 (or additionally, as will be discussed hereinafter, its displacement along the vertical axis z).

The actuation structure <NUM> comprises, in each quadrant in which it is possible to divide the microelectromechanical device <NUM>: a first pair of driving arms 22a, arranged externally to the connecting arms 15b, between the same connecting arms 15b and the frame <NUM>' (being separated therefrom by portions of the aforesaid cavity <NUM>); and a second pair of driving arms 22b, arranged internally to the connecting arms 15b, between the same connecting arms 15b and a corresponding lever element <NUM> (being separated therefrom by further portions of the aforesaid cavity <NUM>). In the embodiment illustrated, the driving arms 22a, 22b have a generically trapezoidal (or fin) shape in the horizontal plane xy.

Each driving arm 22a, 22b is suspended in cantilever fashion above the cavity <NUM> and carries, at a top surface thereof (opposite to the same cavity <NUM>) a respective piezoelectric material region <NUM> (in particular of PZT - lead zirconate titanate), having substantially the same extension in the horizontal plane xy as the driving arm 22a, 22b (for example, and in a way not highlighted in the figures for simplicity, the piezoelectric material regions <NUM> may have a dimension smaller by approximately <NUM> for each side than the underlying driving arm 22a, 22b).

In a possible implementation, the driving arms 22a, 22b are shaped so as to provide substantially a same piezoelectric actuation area as a result of biasing of the respective piezoelectric material regions <NUM>.

Each driving arm 22a, 22b has a respective first end fixedly coupled to a corresponding connecting arm 15b (and, therefore, fixed with respect to the frame <NUM>') and a respective second end elastically coupled to the corresponding lever element <NUM>.

In detail, the driving arms 22a of the first pair are elastically coupled to the corresponding lever element <NUM>, at its second end (in the proximity of the frame <NUM>'), by first elastic driving elements <NUM>, which extend externally to the elastic connecting elements <NUM>, between the same elastic connecting elements <NUM> and the frame <NUM>'; and the driving arms 22b of the second pair are elastically coupled to the corresponding lever element <NUM> by second elastic driving elements <NUM>, which extend internally to the elastic connecting elements <NUM>, between the same elastic connecting elements <NUM> and the tiltable structure <NUM>.

The first and second elastic driving elements <NUM>, <NUM> therefore extend on opposite sides of the elastic connecting elements <NUM> with respect to the lever rotation axis L and are each constituted by a respective folded elastic element, having a high rigidity in regard to movements out of the horizontal plane xy (along the orthogonal axis z) and are compliant to torsion (about a rotation axis parallel to their direction of extension, transverse to the corresponding lever element <NUM>).

During operation, as on the other hand will be evident from an examination of <FIG>, biasing (for example with a positive voltage difference ΔV) of the piezoelectric material regions <NUM> carried by the driving arms 22a of the first pair causes an upwards displacement (along the vertical axis z) of the respective second end elastically coupled to the corresponding lever element <NUM>; this displacement is transmitted by the first elastic driving elements <NUM>, thus causing upwards displacement of the second end of the lever element <NUM> and rotation of the same lever element <NUM> about the lever rotation axis L, leading to a corresponding downwards displacement of the first end and, therefore, of the coupled edge portion of the tiltable structure <NUM>.

This rotation of the lever element <NUM> is not hindered - but rather enabled - by the second elastic driving elements <NUM> and occurs, for example, with a zero biasing (for example, with a zero-voltage difference ΔV) of the piezoelectric material regions <NUM> carried by the driving arms 22b of the second pair.

Likewise, biasing (for example, once again with a positive voltage difference ΔV) of the piezoelectric material regions <NUM> carried by the driving arms 22b of the second pair causes an upwards displacement (along the vertical axis z) of the respective second end elastically coupled to the corresponding lever element <NUM>; this displacement is transmitted by the second elastic driving elements <NUM>, thus causing upwards displacement of the first end of the lever element <NUM> and rotation of the same lever element <NUM> about the lever rotation axis L, leading to a corresponding upwards displacement of the second end and, therefore, of the coupled edge portion of the tiltable structure <NUM>.

The above rotation of the lever element <NUM> is not hindered - but rather enabled - in this case by the first elastic driving elements <NUM> and occurs for example with a zero biasing (for example, with a zero-voltage difference ΔV) of the piezoelectric material regions <NUM> carried by the driving arms 22a of the first pair.

In a possible embodiment, the piezoelectric material regions <NUM> of the driving arms 22a of the first pair in a given one of the quadrants into which the microelectromechanical device <NUM> is divided are electrically connected (in a manner not illustrated, by appropriate electrical connection elements) to the piezoelectric material regions <NUM> of the driving arms 22b of the second pair in the quadrant of the microelectromechanical device <NUM> arranged symmetrically with respect to the centre O. Likewise, the piezoelectric material regions <NUM> of the driving arms 22b of the second pair in the given one of the quadrants into which the microelectromechanical device <NUM> is divided are electrically connected to the piezoelectric material regions <NUM> of the driving arms 22a of the first pair in the quadrant of the microelectromechanical device <NUM> arranged symmetrically with respect to the centre O.

As a result of the aforesaid electrical connections, four sets of driving electrodes are obtained, which are represented schematically in <FIG> with different shades of grey, from the darkest to the lightest: Set1, Set2, Set3, and Set4. Biasing of the aforesaid sets of driving electrodes allows to obtain desired rotations of the tiltable structure <NUM> about the first and second rotation axes A1, A2; in a possible non-limiting implementation, it is possible to obtain four different rotations of the tiltable structure <NUM> and four corresponding quasi-static driving positions.

In detail: application of the voltage difference ΔV, for example positive, to the driving electrodes of the sets Set2 and Set3, with zero biasing of the driving electrodes of the sets Set1 and Set4 leads to a negative rotation about the rotation axis A1; application of the voltage difference ΔV to the driving electrodes of the sets Set1 and Set4, with zero biasing of the driving electrodes of the sets Set2 and Set3 leads to a positive rotation about the same rotation axis A1; application of the voltage difference ΔV, for example once again positive, to the driving electrodes of the sets Set1 and Set3, with zero biasing of the driving electrodes of the sets Set2 and Set4 leads to a negative rotation about the rotation axis A2; and application of the voltage difference ΔV to the driving electrodes of the sets Set2 and Set4, with zero biasing of the driving electrodes of the sets Set1 and Set3 leads to a positive rotation about the same rotation axis A2.

By way of example, <FIG> shows the latter position of the tiltable structure <NUM>, with positive rotation about the rotation axis A2, and moreover shows the deformation of the various elastic elements involved in the same rotation, as described in detail previously.

As mentioned, in different implementations, biasing of the four sets of driving electrodes may be such as to cause the tiltable structure <NUM> to assume any position within its range of movement.

<FIG> shows schematically, by way of example, the displacement of the microelectromechanical device <NUM>, along a section IV-IV of <FIG>, with a positive rotation about the rotation axis A2. In <FIG>, F designates the driving force due to the piezoelectric effect acting at the points of coupling of the lever elements <NUM> with the respective elastic driving elements <NUM>, <NUM> (which are, in fact, configured so as to transmit the force in the direction of the vertical axis z to the aforesaid lever elements <NUM>) causing the lever movement of the lever elements <NUM> about the lever rotation axis L; and θ designates the consequent angle of rotation of the tiltable structure <NUM> with respect to the vertical axis z.

As shown schematically in the aforesaid <FIG>, the microelectromechanical device <NUM> further comprises one or more piezoresistive (PZR) sensors <NUM>, appropriately arranged so as to provide one or more detection signals associated to the rotation of the tiltable structure <NUM> about the first and second rotation axes A1, A2; these detection signal can be supplied as a feedback at the output from the microelectromechanical device <NUM> allowing implementing of an appropriate closed control loop.

The above piezoresistive sensors <NUM> are obtained (for example, by surface diffusion of dopant atoms) on one or more of the connecting arms 15b of the connecting structure <NUM> (different arrangements for the piezoresistive sensors <NUM> may, however, be envisaged). Advantageously, the elastic connecting elements <NUM> are able to transmit the stresses to the connecting arms 15b and therefore towards the piezoresistive sensors <NUM>, thus enabling detection of the rotation of the tiltable structure <NUM>.

In a manner not described in detail, but that will be evident, two arrangements of piezoresistive sensors <NUM> may be used, in a Wheatstone-bridge configuration, for detecting rotations of the tiltable structure <NUM> about the first and second rotation axes A1, A2 (and therefore the overall rotation of the tiltable structure <NUM>).

Alternatively, as it is described in detail in the aforementioned document <CIT>, a mechanical amplification structure may moreover be introduced, designed to maximize, by an appropriate lever mechanism, the stress detected by the piezoresistive sensors <NUM> and, therefore, the corresponding sensitivity.

In a manner not illustrated, other types of detection of the rotations of the tiltable structure <NUM> may moreover be provided, for example by means of piezoelectric sensors.

<FIG> shows a simplified sectional view of the microelectromechanical device <NUM>, where some elements are omitted for simplicity and others are represented schematically.

In particular, the above sectional view shows that the frame <NUM>' is coupled at the bottom to a supporting wafer (the so-called "handling wafer") <NUM>, which has, underneath the cavity <NUM> and the tiltable structure <NUM>, a recess <NUM>, for enabling rotation of the same tiltable structure <NUM>.

In this embodiment, the tiltable structure <NUM>, as likewise the actuation structure <NUM>, is made in the active layer <NUM> of a SOI wafer, a supporting layer <NUM> of which, separated from the active layer <NUM> by a dielectric layer <NUM>, is coupled at the bottom to the aforesaid handling wafer <NUM>. The tiltable structure <NUM> moreover has at the bottom, in contact with the surface opposite to the reflecting surface <NUM>', reinforcement elements <NUM>, having extension along the vertical axis z.

As shown in <FIG>, a possible variant embodiment envisages, instead, that the tiltable structure <NUM> is formed at a higher level with respect to the actuation structure <NUM>, in a stacked manner. In particular, in this case the tiltable structure <NUM> is coupled in a stacked manner to a base portion <NUM>, formed at the same level as the actuation structure <NUM> (separated from the latter by the cavity <NUM>), by means of a connection pillar <NUM> having extension along the vertical axis z. In this case, advantageously, an amplification of the lever effect implemented by the lever elements <NUM> (here not illustrated) is obtained, thus achieving a wider angle of inclination of the tiltable structure <NUM>, with a more compact and sturdier solution.

The tiltable structure <NUM> is formed in this case in a different wafer of semiconductor material, which can be coupled to the base surface <NUM> for example by wafer bonding in front-end stages of the manufacturing process.

The advantages of the present solution emerge clearly from the foregoing description.

In any case, it is highlighted that the described solution provides robust and efficient microelectromechanical mirror devices, in particular of the bi-dimensional vector-scanning type (the so-called vector scanning MEMS).

The solution described has a high linearity, wide angles of aperture for rotation of the mirror, and a compact structure.

For example, the microelectromechanical device <NUM> can be advantageously used in a projection apparatus <NUM> designed to be operatively coupled to a portable electronic apparatus <NUM>, as illustrated schematically with reference to <FIG>.

The projection apparatus <NUM> comprises a source <NUM>, designed to generate an image <NUM>; the microelectromechanical device <NUM>, acting as mirror and designed to receive the image <NUM> and to direct it towards a screen <NUM> (external to, and set at a distance from, the same projection apparatus <NUM>); a first driving circuit <NUM>, designed to provide driving signals to the source <NUM>, for generation of the image <NUM> to be projected; a second driving circuit <NUM>, designed to supply driving signals to the actuation structure <NUM> of the microelectromechanical device <NUM>; and a communication interface <NUM>, designed to receive, from an external control unit <NUM>, for example included in the portable electronic apparatus <NUM>, information on the image to be projected, for example in the form of an array of pixels, which are sent at an input of the source <NUM> for driving it.

Finally, it is clear that modifications and variations may be made to what has been described and illustrated herein, without thereby departing from the scope of the present invention, as defined in the appended claims.

In particular, the present solution can also be used to provide actuators for microelectromechanical speaker devices (the so-called µ-speakers), by varying the combination of biasing of the piezoelectric material regions <NUM> carried by the driving arms 22a, 22b of the first and second pairs.

In this case, the piezoelectric material regions <NUM> of the driving arms 22a of the first pairs are electrically connected together, and moreover the piezoelectric material regions <NUM> of the driving arms 22b of the second pairs are electrically connected together.

With reference to <FIG>, by applying a same voltage difference ΔV, for example positive, to the driving electrodes 22b of the second pairs, with zero biasing of the driving electrodes 22a of the first pairs, an upwards displacement along the vertical axis z of the tiltable structure <NUM> is obtained. Likewise, by applying a same voltage difference ΔV to the driving electrodes 22a of the first pairs, with zero biasing of the driving electrodes 22b of the second pairs, a downwards displacement along the vertical axis z of the same tiltable structure <NUM> is obtained.

Basically, a piston-like displacement is achieved for the tiltable structure <NUM>, which can thus be used as actuator, for example coupled to an appropriate deformable membrane (in a manner not illustrated), for generation of sound waves in a microelectromechanical speaker device.

Advantageously, this solution allows to obtain vertical movements of the tiltable structure <NUM>, with high linearity and excellent resistance to stress and shocks.

Furthermore, it is evident that variants may be envisaged as regards the shape and arrangement of the elements that constitute the microelectromechanical device <NUM>, for example different shapes of the tiltable structure <NUM> (and of the corresponding reflecting surface <NUM>').

In this regard, <FIG> shows a further embodiment of the microelectromechanical device <NUM>, which differs from the one illustrated previously in that the rotation axes A1 and A2 are inclined by <NUM>° with respect to the first and second horizontal axes x and y, i.e., to the sides of the frame <NUM>' of the fixed structure <NUM> and of the corresponding die.

Consequently, the lever elements <NUM> are in this case aligned with the aforesaid horizontal axes x and y, whereas the central arms 15a of the supporting structure <NUM> are oriented along the diagonal directions (i.e., in this case, along the aforesaid rotation axes A1 and A2).

The tiltable structure <NUM> moreover has here a substantially square shape in the horizontal plane xy and the first portion 18a, once again of a folded type, of each of the elastic suspension elements <NUM> is doubled and connected to two end portions of a respective side of the tiltable structure <NUM>.

In addition, in the embodiment illustrated, the first and second elastic decoupling elements <NUM>, <NUM> have a linear and non-folded arrangement, being in each case rigid to movements out of the horizontal plane xy and compliant to rotation.

Otherwise, the configuration and operation of the microelectromechanical device <NUM> does not differ substantially from what has been discussed previously for the first embodiment.

Claim 1:
A microelectromechanical device (<NUM>), comprising:
a fixed structure (<NUM>) having a frame (<NUM>') defining a cavity (<NUM>);
a tiltable structure (<NUM>) elastically suspended above the cavity (<NUM>) and having a main extension in a horizontal plane (xy) ;
a piezoelectrically driven actuation structure (<NUM>), configured to be biased to cause a desired rotation of the tiltable structure (<NUM>) about a first rotation axis (A1) and a second rotation axis (A2) in said horizontal plane (xy); and
a supporting structure (<NUM>) integral with the fixed structure (<NUM>) and extending in the cavity (<NUM>) starting from the frame (<NUM>'),
further comprising lever elements (<NUM>), elastically coupled to the tiltable structure (<NUM>) at a first end by respective elastic suspension elements (<NUM>) of the microelectromechanical device (<NUM>) and to the supporting structure (<NUM>) at a second end by elastic connecting elements (<NUM>) of the microelectromechanical device (<NUM>), of a torsional type, which define a lever rotation axis (L),
wherein the lever elements (<NUM>) are moreover elastically coupled to the actuation structure (<NUM>) so that biasing of said actuation structure (<NUM>) causes, as a result of rotation of said lever elements (<NUM>) about the lever rotation axis (L), the desired rotation of the tiltable structure (<NUM>) about the first rotation axis (A1) and the second rotation axis (A2);
characterised in that said actuation structure (<NUM>) comprises, for each of said lever elements (<NUM>), a first pair of driving arms (22a), elastically coupled to the lever element (<NUM>) by first elastic driving elements (<NUM>) of the microelectromechanical device (<NUM>), and a second pair of driving arms (22b), elastically coupled to the lever element (<NUM>) by second elastic driving elements (<NUM>) of the microelectromechanical device (<NUM>) on an opposite side of the lever rotation axis (L) with respect to said first elastic driving elements (<NUM>).