AN OPHTHALMIC PROGRESSIVE ADDITION LENS FOR AN EMMETROPIC AND PRESBYOPIC WEARER; METHOD FOR PROVIDING SUCH A LENS

Abstract

An ophthalmic progressive addition lens for an emmetropic and presbyopic wearer having a mean refractive power, PPO(α, β), a module of resulting astigmatism, ASR(α, β), an acuity loss value ACU(α, β), wherein the (α, β) functions are determined in as-worn conditions of the lens by the wearer, and a first acuity criterion, AcuityCriterion1 which fulfils following requirement: AcuityCriterion1≥435 D2·deg2, and wherein: AcuityCriterion1 is defined as a combination of PPO(α, β), ASR(α, β), ADDp, and ACU(α, β).

Description

The invention relates generally to the field of vision improvement and more specifically concerns an ophthalmic progressive addition lens for an emmetropic and presbyopic wearer. It also relates to a method for providing such a lens.

Conventionally, spectacles lenses are manufactured on request in accordance with specifications intrinsic to individual wearers. Such specifications generally encompass a medical prescription made by an ophthalmologist or an eye care practitioner.

An emmetropic wearer has an optical power correction for far vision which is near to nil. According to the present invention, one considers that a emmetropic wearer has a prescribed far vision mean refractive power which is greater than minus 1 Diopter and less than plus 1 Diopter. For presbyopic wearers, the value of the power correction is different for far vision and near vision, due to the difficulties of accommodation in near vision. The prescription thus comprises a far-vision power value and an addition representing the power increment between far vision and near vision. The addition is qualified as prescribed addition ADD_p.

The inventors have noticed that current ophthalmic progressive addition lens for an emmetropic and presbyopic wearer can still be improved so as to enhance the wearer's visual comfort.

A problem that the invention aims to solve is thus to enhance the wearer's visual comfort.

For this purpose, a subject of the invention is an ophthalmic progressive addition lens for an emmetropic and presbyopic wearer which has a prescribed far vision mean refractive power greater than minus 1 Diopter and less than plus 1 Diopter and a non nil prescribed addition, ADD_p, said lens having a mean refractive power, PPO(α, β), a module of resulting astigmatism, ASR(α, β), an acuity loss value ACU(α, β), where said (α, β) functions are determined in as-worn conditions of the lens by the wearer, and a first acuity criterion, AcuityCriterion1 which fulfils following requirement:

AcuityCriterion1≥435 D²·deg²

and where, “D” refers to Diopter, “deg” to degree, AcuityCriterion1 is defined as a combination of PPO(α, β), ASR(α, β), ADD_p, and ACU(α, β).

According to an embodiment, AcuityCriterion1 fulfils following requirement: AcuityCriterion1≥465 D²·deg².

According to an embodiment, AcuityCriterion1 fulfils following requirement: AcuityCriterion1≥495 D²·deg².

The inventors have discovered that to defining a threshold value of an acuity criterion is suitable to characterize ophthalmic progressive addition lens for an emmetropic and presbyopic wearer where the wearer's visual comfort is enhanced in view of known prior art ophthalmic progressive addition lens.

According to different embodiments of the present invention, that may be combined:

• • the lens is further characterized by a meridian line, ML(α, β), a fitting cross, FC(α_FC, β_FC), said (α, β) functions being determined in as-worn conditions of the lens by the wearer for gaze directions (α, β) joining the center of rotation of the eye, CRE, and the lens, where α is a lowering angle in degree and β is an azimuth angle in degree and wherein: the acuity loss value ACU(α, β) is expressed in log MAR and defined according to following equation:

ACU(α,β)=−log(AC%(α,β)/100), where:

• • • AC %(α, β)=100−63×P(α, β)−44.3×ASR(α, β)+7.2×P(α, β)²+19.5×P(α, β)×ASR(α, β)+ASR(α, β)²; when P(α, β)≥0; and
    • AC %(α, β)=100−44.3×ASR(α, β)+ASR(α, β)²; when P(α, β)<0;
    • P(α, β)=PPO(α, β)−PPO(α,β_α_mer);
    • β_α_mer is the value of the azimuth angle β on the meridian line, ML(α, β), at the lowering angle α;
  • and where AcuityCriterion1=Numerator1/Denominator;
    • Numerator1=LAcuSub85(0.1)×LAcuAlpha85(0.1)×ADD_p⁴;
    • Denominator=AsrGradMax×PeaksMean×PVL²;
    • LAcuSub85(0.1) is the angular extent (in deg²) of the zone where ACU(α, β)≤0.1 log MAR, inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees, and where α≥α85%, α85% being the lowering angle where 85% of the prescribed addition is perceived by the wearer on the meridian line;
    • LAcuAlpha85(0.1) is the acuity width (in deg) at α85% between two iso-acuity loss lines corresponding to 0.1 log MAR and is equal to β₊(ACU(α85%, β)=0.1)−β₋(ACU(α85%, β)=0.1), where β₊ is greater than β_α_mer(α85%) and β₋ is less than β_α_mer(α85%);
    • PVL is the power variation length is expressed in deg and defined as being equal to (α85%−α15%), α15% being the lowering angle where 15% of the prescribed addition is perceived by the wearer on the meridian line;
    • AsrGradMax is the maximum value of the norm of the gradient of resulting astigmatism, ASR(α, β), expressed in Diopter per degree, calculated inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees;
    • PeaksMean is the mean maximum module of resulting astigmatism (in Diopter) which is equal to [ASR_max(α_L, β_L)+ASR_max(α_R, β_R)]/2, where ASR_max(α_L, β_L) is the maximum module of resulting astigmatism on a side (left side) of the meridian line, and ASR_max(α_R, β_R) is the maximum module of resulting astigmatism on the other side (right side) of the meridian line that are both determined inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees;
  • a second acuity criterion, AcuityCriterion2, fulfils following requirement:

AcuityCriterion2≥1110 D²·deg², where:

• • • AcuityCriterion2=Numerator2/Denominator;
    • Numerator2=LAcuSub85(0.2)×LAcuAlpha85(0.2)×ADD_p⁴;
    • LAcuSub85(0.2) is the angular extent (in deg²) of the zone where ACU(α, β)≤0.2 log MAR, inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees, and where α≥α85%;
    • LAcuAlpha85(0.2) is the acuity width (in deg) at α85% between two iso-acuity loss lines corresponding to 0.2 log MAR and is equal to β₊(ACU(α85%, β)=0.2)−β₋(ACU(α85%, β)=0.2), where β₊ is greater than β_α_mer(α85%) and β₋ is less than β_α_mer(α85%);
    • According to an embodiment, AcuityCriterion2 fulfils following requirement: AcuityCriterion2≥1130 D²·deg².
    • According to an embodiment, AcuityCriterion2 fulfils following requirement: AcuityCriterion2≥1150 D²·deg².
  • a third acuity criterion, AcuityCriterion3, fulfils following requirement:

AcuityCriterion3≥37.4 D·deg, where:

• • • AcuityCriterion3=Numerator3/Denominator;
    • Numerator3=LAcuSubFC(0.1)×ADD_p³;
    • LAcuSubFC(0.1) is the angular extent (in deg²) of the zone where ACU(α, β)≤0.1 log MAR, inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees, and where α≥α_FC;
    • According to an embodiment, AcuityCriterion3 fulfils following requirement: AcuityCriterion3≥37.8 D·deg.
    • According to an embodiment, AcuityCriterion3 fulfils following requirement: AcuityCriterion3≥38 D·deg.
  • a fourth acuity criterion, AcuityCriterion4, fulfils following requirement:

AcuityCriterion4≥58.4 D·deg, where:

• • • AcuityCriterion4=Numerator4/Denominator;
    • Numerator4=LAcuSubFC(0.2)×ADD_p³;
    • LAcuSubFC(0.2) is the angular extent (in deg²) of the zone where ACU(α, β)≤0.2 log MAR, inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees, and where α≥α_FC;
    • According to an embodiment, AcuityCriterion4 fulfils following requirement: AcuityCriterion4≥59.2 D·deg.
    • According to an embodiment, AcuityCriterion4 fulfils following requirement: AcuityCriterion4≥60 D·deg.
  • a fifth acuity criterion, AcuityCriterion5, fulfils following requirement:

AcuityCriterion5≥85 D·deg, where:

• • • AcuityCriterion5=Numerator5/Denominator;
    • Numerator5=LAcuDomain(0.1)×ADD_p³;
    • LAcuDomain(0.1) is the angular extent (in deg²) of the zone where ACU(α, β)≤0.1 log MAR, inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees; According to an embodiment, AcuityCriterion5 fulfils following requirement: AcuityCriterion5≥85.5 D·deg.
    • According to an embodiment, AcuityCriterion5 fulfils following requirement: AcuityCriterion5≥86 D·deg.
  • a sixth acuity criterion, AcuityCriterion6, fulfils following requirement:

AcuityCriterion6≥117.5 D·deg, where:

• • • AcuityCriterion6=Numerator6/Denominator;
    • Numerator6=LAcuDomain(0.2)×ADD_p³;
    • LAcuDomain(0.2) is the angular extent (in deg²) of the zone where ACU(α, β)≤0.2 log MAR, inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees.
    • According to an embodiment, AcuityCriterion6 fulfils following requirement: AcuityCriterion6≥118.3 D·deg.
    • According to an embodiment, AcuityCriterion6 fulfils following requirement: AcuityCriterion6≥119 D·deg.

In another aspect, the present invention also provides a method implemented by computer means for providing an ophthalmic progressive addition lens to an emmetropic and presbyopic wearer having a prescribed far vision mean refractive power greater than minus 1 Diopter and less than plus 1 Diopter and a non nil prescribed addition, ADD_p, comprising the step of calculating a mean refractive power repartition, PPO(α, β), a module of resulting astigmatism repartition, ASR(α, β), an acuity loss value repartition ACU(α, β), where said (α, β) functions are calculated in as-worn conditions of the lens by the wearer, so as to fulfil following requirement of a first acuity criterion, AcuityCriterion1:

AcuityCriterion1≥435 D²·deg²;

Where, “D” refers to Diopter, “deg” to degree, AcuityCriterion1 is defined as a combination of PPO(α, β), ASR(α, β), ADD_p, and ACU(α, β).

According to different embodiments of the method of the present invention, that may be combined:

• • the method further comprising following steps:
    • Calculating or defining a meridian line, ML(α, β),
    • Calculating or defining a fitting cross, FC(α_FC, β_FC),
    • Calculating the mean refractive power, PPO(α, β), and the module of resulting astigmatism, ASR(α, β), determined in as-worn conditions of the lens by the wearer for gaze directions (α, β) joining the center of rotation of the eye, CRE, and the lens, where α is a lowering angle in degree and β is an azimuth angle in degree, an acuity loss value ACU(α, β) is expressed in log MAR and defined according to following equation:

ACU(α,β)=−log(AC%(α,β)/100), where:

• • • • AC %(α, β)=10063×P(α, β)−44.3×ASR(α, β)+7.2×P(α, β)²+19.5×P(α, β)×ASR(α, β)+ASR(α, β)²; when P(α, β)≥0; and
      • AC %(α, β)=100−44.3×ASR(α, β)+ASR(α, β)²; when P(α, β)<0;
      • P(α, β)=PPO(α, β)−PPO(α,β_α_mer);
      • β_α_mer is the value of the azimuth angle β on the meridian line, ML(α, β), at the lowering angle α;
    • and where AcuityCriterion1=Numerator1/Denominator;
      • Numerator1=LAcuSub85(0.1)×LAcuAlpha85(0.1)×ADD_p⁴;
      • Denominator=AsrGradMax×PeaksMean×PVL²;
      • LAcuSub85(0.1) is the angular extent (in deg²) of the zone where ACU(α, β)≤0.1 log MAR, inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees, and where α≥α85%, α85% being the lowering angle where 85% of the prescribed addition is perceived by the wearer on the meridian line;
      • LAcuAlpha85(0.1) is the acuity width (in deg) at α85% between two iso-acuity loss lines corresponding to 0.1 log MAR and is equal to:
        • β₊(ACU(α85%, β)=0.1)=β₋(ACU(α85%, β)=0.1), where β₊ is greater than β_α_mer(α85%) and β₋ is less than β_α_mer(α85%);
      • PVL is the power variation length is expressed in deg and defined as being equal to (α85%−α15%), α15% being the lowering angle where 15% of the prescribed addition is perceived by the wearer on the meridian line;
      • AsrGradMax is the maximum value of the norm of the gradient of resulting astigmatism, ASR(α, β), expressed in Diopter per degree, calculated inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees;
      • PeaksMean is the mean maximum module of resulting astigmatism (in Diopter) which is equal to [ASR_max(α_L, β_L)+ASR_max(α_R, β_R)]/2, where ASR_max(α_L, β_L) is the maximum module of resulting astigmatism on a side (left side) of the meridian line, and ASR_max(α_R, β_R) is the maximum module of resulting astigmatism on the other side (right side) of the meridian line that are both determined inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees;
  • one calculates the lens so as to fulfil following requirement of a second acuity criterion, AcuityCriterion2:

AcuityCriterion2≥1100 D²·deg², where:

• • • AcuityCriterion2=Numerator2/Denominator;
    • Numerator2=LAcuSub85(0.2)×LAcuAlpha85(0.2)×ADD_p⁴;
    • LAcuSub85(0.2) is the angular extent (in deg²) of the zone where ACU(α, β)≤0.2 log MAR, inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees, and where α≥α85%;
    • LAcuAlpha85(0.2) is the acuity width (in deg) at α85% between two iso-acuity loss lines corresponding to 0.2 log MAR and is equal to β₊(ACU(α85%, β)=0.2)−β₋(ACU(α85%, β)=0.2), where β₊ is greater than β_α_mer(α85%) and β₋ is less than β_α_mer(α85%);
  • one calculates the lens so as to fulfil following requirement of a third acuity criterion, AcuityCriterion3:

AcuityCriterion3≥37.4 D·deg, where:

• • • AcuityCriterion3=Numerator3/Denominator;
    • Numerator3=LAcuSubFC(0.1)×ADD_p³;
    • LAcuSubFC(0.1) is the angular extent (in deg²) of the zone where ACU(α, β)≤0.1 log MAR, inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees, and where α≥α_FC;
  • one calculates the lens so as to fulfil following requirement of a fourth acuity criterion, AcuityCriterion4:

AcuityCriterion4≥58.4 D·deg, where:

• • • AcuityCriterion4=Numerator4/Denominator;
    • Numerator4=LAcuSubFC(0.2)×ADD_p³;
    • LAcuSubFC(0.2) is the angular extent (in deg²) of the zone where ACU(α, β)≤0.2 log MAR, inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees, and where α≥α_FC;
  • one calculates the lens so as to fulfil following requirement of a fifth acuity criterion, AcuityCriterion5:

AcuityCriterion5≥85 D·deg, where:

• • • AcuityCriterion5=Numerator5/Denominator;
    • Numerator5=LAcuDomain(0.1)×ADD_p³;
    • LAcuDomain(0.1) is the angular extent (in deg²) of the zone where ACU(α, β)≤0.1 log MAR, inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees;
  • one calculates the lens so as to fulfil following requirement of a sixth acuity criterion, AcuityCriterion6:

AcuityCriterion6≥117.5 D·deg, where:

• • • AcuityCriterion6=Numerator6/Denominator;
    • Numerator6=LAcuDomain(0.2)×ADD_p³;
    • LAcuDomain(0.2) is the angular extent (in deg²) of the zone where ACU(α, β)≤0.2 log MAR, inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees;
  • here above requirements of preferred embodiments directed to AcuityCriterion1 and/or AcuityCriterion2 and/or AcuityCriterion3 and/or AcuityCriterion4 and/or AcuityCriterion5 and/or AcuityCriterion6 may be chosen within the scope of the method of the present invention.
  • the method comprises an optimization routine where at least a target is chosen within requirement of an acuity criterion chosen in the list consisting of AcuityCriterion1, AcuityCriterion2, AcuityCriterion3, AcuityCriterion4, AcuityCriterion5, AcuityCriterion6.

In still another aspect, the present invention relates to a computer program product comprising one or more stored sequence of instruction that is accessible to a processor and which, when executed by the processor, causes the processor to carry out at least one of the steps of the different embodiments of the preceding method.

The invention also relates to a computer-readable medium carrying one or more sequences of instructions of the preceding computer program product.

DESCRIPTION OF THE DRAWINGS

The features of the present invention, as well as the invention itself, both as to its structure and its operation, will be best understood from the accompanying non limiting drawings and examples, taken in conjunction with the accompanying description, in which:

FIGS. 1 and 2 show, diagrammatically, optical systems of eye and lens and ray tracing from the center of rotation of the eye;

FIG. 3 shows field vision zones of an ophthalmic progressive addition lens;

FIGS. 4 to 14 show diagrams helping understanding the definitions of the criteria used within the frame of the present invention;

FIGS. 15 to 18 give optical characteristics of an ophthalmic progressive addition lens according to the prior art;

FIGS. 19 to 22 give optical characteristics of an ophthalmic progressive addition lens according to the invention.

On the figures, following references correspond to followings:

• • MER is the meridian line;
  • NVGD is the near vision gaze direction;
  • FVGD is the far vision gaze direction;
  • FCGD is the fitting cross gaze direction

Definitions

The following definitions are provided so as to define the wordings used within the frame of the present invention.

The wordings “wearer's prescription”, also called “prescription data”, are known in the art. Prescription data refers to one or more data obtained for the wearer and indicating for at least an eye, preferably for each eye, a prescribed sphere SPH_p, and/or a prescribed astigmatism value CYL_p and a prescribed axis AXIS_p suitable for correcting the ametropia of each eye for the wearer and, if suitable, a prescribed addition ADD_p suitable for correcting the presbyopia of each of his eyes.

“Progressive ophthalmic addition lenses” are known in the art. According to the invention, the lens may be a standard lens but also a lens for information glasses, wherein the lens comprises means for displaying information in front of the eye. The lens may also be suitable for sunglasses or not. All ophthalmic lenses of the invention may be paired so as to form a pair of lenses (left eye LE, right eye RE).

A “gaze direction” is identified by a couple of angle values (α,β), wherein said angles values are measured with regard to reference axes centered on the center of rotation of the eye, commonly named as “CRE”. More precisely, FIG. 1 represents a perspective view of such a system illustrating parameters α and β used to define a gaze direction. FIG. 2 is a view in the vertical plane parallel to the antero-posterior axis of the wearer's head and passing through the center of rotation of the eye in the case when the parameter β is equal to 0. The center of rotation of the eye is labeled CRE. The axis CRE-F′, shown on FIG. 2 in a dot-dash line, is the horizontal axis passing through the center of rotation of the eye and extending in front of the wearer that is the axis CRE-F′ corresponding to the primary gaze direction. The lens is placed and centered in front of the eye such that the axis CRE-F′ cuts the front surface of the lens on a point called the fitting cross, which is, in general, present on lenses to enable the positioning of lenses in a frame by an optician. The point of intersection of the rear surface of the lens and the axis CRE-F′ is the point, O. A vertex sphere, which center is the center of rotation of the eye, CRE, and has a radius q′=O−CRE, intercepts the rear surface of the lens in a point of the horizontal axis. A value of radius q′ of 25.5 mm corresponds to a usual value and provides satisfying results when wearing the lenses. Other value of radius q′ may be chosen. A given gaze direction, represented by a solid line on FIG. 1, corresponds to a position of the eye in rotation around CRE and to a point J (see FIG. 2) of the vertex sphere; the angle β is the angle formed between the axis CRE-F′ and the projection of the straight line CRE-J on the horizontal plane comprising the axis CRE-F′; this angle appears on the scheme on FIG. 1. The angle α is the angle formed between the axis CRE-J and the projection of the straight line CRE-J on the horizontal plane comprising the axis CRE-F′; this angle appears on the scheme on FIGS. 1 and 2. A given gaze view thus corresponds to a point J of the vertex sphere or to a couple (α,β). The more the value of the lowering gaze angle is positive, the more the gaze is lowering and the more the value is negative, the more the gaze is rising. In a given gaze direction, the image of a point M in the object space, located at a given object distance, is formed between two points S and T corresponding to minimum and maximum distances JS and JT, which would be the sagittal and tangential local focal lengths. The image of a point in the object space at infinity is formed, at the point F′. The distance D corresponds to the rear frontal plane of the lens.

For each gaze direction (α,β), a mean refractive power PPO(α,β), a module of astigmatism ASR(α,β) and an axis AXE(α,β) of this astigmatism, and a module of resulting (also called residual or unwanted) astigmatism ASR(α,β) are defined.

“Astigmatism” refers to astigmatism generated by the lens, or to residual astigmatism (resulting astigmatism) which corresponds to the difference between the prescribed astigmatism (wearer astigmatism) and the lens-generated astigmatism; in each case, with regards to amplitude or both amplitude and axis;

“Ergorama” is a function associating to each gaze direction the usual distance of an object point. Typically, in far vision following the primary gaze direction, the object point is at infinity. In near vision, following a gaze direction essentially corresponding to an angle α of the order of 35° and to an angle β of the order of 5° in absolute value towards the nasal side, the object distance is of the order of 30 to 50 cm. For more details concerning a possible definition of an ergorama, U.S. Pat. No. 6,318,859 may be considered. This document describes an ergorama, its definition and its modeling method. For a method of the invention, points may be at infinity or not. Ergorama may be a function of the wearer's ametropia. Using these elements, it is possible to define a wearer optical power and astigmatism, in each gaze direction. An object point M at an object distance given by the ergorama is considered for a gaze direction (α,β). An object proximity ProxO is defined for the point M on the corresponding light ray in the object space as the inverse of the distance MJ between point M and point J of the vertex sphere:

ProxO=1/MJ

This enables to calculate the object proximity within a thin lens approximation for all points of the vertex sphere, which is used for the determination of the ergorama. For a real lens, the object proximity can be considered as the inverse of the distance between the object point and the front surface of the lens, on the corresponding light ray.For the same gaze direction (α,β), the image of a point M having a given object proximity is formed between two points S and T which correspond respectively to minimal and maximal focal distances (which would be sagittal and tangential focal distances). The quantity ProxI is called image proximity of the point M:

$\mathrm{Pr}\mathrm{oxI}=\frac{1}{2}\left(\frac{1}{\mathrm{JT}}+\frac{1}{\mathrm{JS}}\right)$

By analogy with the case of a thin lens, it can therefore be defined, for a given gaze direction and for a given object proximity, i.e. for a point of the object space on the corresponding light ray, an optical power PPO as the sum of the image proximity and the object proximity.

PPO=ProxO+ProxI

The optical power is also called refractive power.With the same notations, an astigmatism AST is defined for every gaze direction and for a given object proximity as:

$\mathrm{AST}=\frac{1}{\mathrm{JT}}-\frac{1}{\mathrm{JS}}$

This definition corresponds to the astigmatism of a ray beam created by the lens. The resulting astigmatism ASR is defined for every gaze direction through the lens as the difference between the actual astigmatism value AST for this gaze direction and the prescribed astigmatism for the same lens. The residual astigmatism (resulting astigmatism) ASR more precisely corresponds to module of the vectorial difference between actual (AST, AXE) and prescription data (CYL_p, AXIS_p).

When the characterization of the lens is of optical kind, it refers to the ergorama-eye-lens system described above. For simplicity, the term ‘lens’ is used in the description but it has to be understood as the ‘ergorama-eye-lens system’. The values in optic terms can be expressed for gaze directions. Conditions suitable to determine of the ergorama-eye-lens system are called in the frame present invention “as-worn conditions”.

In the remainder of the description, terms like «up», «bottom», «horizontal», «vertical», «above», «below», or other words indicating relative position may be used. These terms are to be understood in the wearing conditions of the lens. Notably, the “upper” part of the lens corresponds to a negative lowering angle α<0° and the “lower” part of the lens corresponds to a positive lowering angle α>0°.

A “far-vision gaze direction”, referred as FVGD, is defined for a lens, as the vision gaze direction corresponding to the far vision (distant) reference point and thus (α_FV, β_FV), where the mean refractive power is substantially equal to the mean prescribed power in far vision, the mean prescribed power being equal to SPH_p+(CYL_p/2). Within the present disclosure, far-vision is also referred to as distant-vision.

A “near-vision gaze direction”, referred as NVGD, is defined for a lens, as the vision gaze direction corresponding to the near vision (reading) reference point, and thus (α_NV, β_NV), where the refractive power is substantially equal to the prescribed power in far vision plus the prescribed addition, ADD_p.

A “fitting-cross gaze direction”, referred as FCGD, is defined for a lens, as the vision gaze direction corresponding to the fitting cross reference point and thus (α_FC, β_FC).

The “meridian line”, referred as ML(α,β), of a progressive lens is a line defined from top to bottom of the lens and passing through the fitting cross where one can see clearly an object point. Said meridian line is defined on the basis of the repartition of module of resulting astigmatism, ASR, over the (α, β) domain and substantially correspond to the center of the two central iso-module of resulting astigmatism values which value is equal to 0.25 Diopter. To be more specific and according to the present invention the meridian line is calculated according to following method:

• • One defines the gaze direction, FCGD, corresponding to the fitting cross (α_FC, β_FC);
  • One calculates the lowering angle α_NV corresponding to the near vision gaze direction;
  • For each lowering angle α comprised between α_FC and α_NV, one calculates the azimuth angle β corresponding to the midway direction between the two central iso-module of resulting astigmatism values which value is equal to 0.25 Diopter; said calculated directions are referred as (α_i, β_i); one calculates a straight line, d2, so as to minimizes the deviation of (α_i, β_i) to said straight line, according to following equation:

$d2:\beta \left(\alpha \right)=a_2\alpha +b_2;{\alpha }_{\mathrm{FC}}<\alpha <{\alpha }_{\mathrm{NV}}$ $a_2,b_2:\min \left\{\sum _i{\left(a_2{\alpha }_i+b_2-{\beta }_i\right)}^2\right\}$

• • where «min″ function relates to determining the a₂ and b₂ parameters so as to minimize the equation between brackets.
  • One calculates a pivot direction (α_piv, β_piv) defined as the intersection between the straight line d2 and a line corresponding to β=β_FC, where

$:\{\begin{array}{c}{\alpha }_{\mathrm{PIV}}=\frac{\left({\beta }_{\mathrm{FC}}-b_2\right)}{a_2}\\ {\beta }_{\mathrm{PIV}}={\beta }_{\mathrm{FC}}\end{array}$

• • One calculates a straight line, d1, where: d1: β(α)=β_piv; α<α_piv;
  • One determines β_NV as being the azimuth angle β of straight line d2 for α_NV; where: β_NV=a₂α_NV+b₂;
  • For each lowering angle α greater than α_NV, one determines the azimuth angle β corresponding to the midway direction between the two central iso-module of resulting astigmatism values which value is equal to 0.25 Diopter; said calculated directions are referred as (α_j, β_j); one calculates a straight line, d3, so as to minimizes the deviation of (α_j, β_j) to said straight line and that passes at the direction (α_NV, β_NV); if the calculated slope is negative, the sloped is chosen to be nil; d3 is thus defined according to following equation:

$d3:\beta \left(\alpha \right)=a_3\left(\alpha -{\alpha }_{\mathrm{NV}}\right)+{\beta }_{\mathrm{NV}};{\alpha }_{\mathrm{NV}}<\alpha a_3,:\min \left\{\sum _j{\left(a_3\left({\alpha }_j-{\alpha }_{\mathrm{NV}}\right)+{\beta }_{\mathrm{NV}}-{\beta }_j\right)}^2;a_3\ge 0\right\}$

• • The meridian line is finally defined as being the line built when following the three segments d1, d2, d3.

“Micro-markings” also called “alignment reference marking” have been made mandatory on progressive lenses by the harmonized standards ISO 13666:2012 (“Alignment reference marking: permanent markings provided by the manufacturer to establish the horizontal alignment of the lens or lens blank, or to re-establish other reference points”) and ISO 8990-2 (“Permanent marking: the lens has to provide at least following permanent markings: alignment reference markings comprising two markings distant from 34 mm one of each other, equidistant from a vertical plane passing through the fitting cross or the prism reference point”). Micro-markings that are defined the same way are also usually made on complex surfaces, such as on a front surface of a lens with a front surface comprising a progressive or regressive front surface.

“Temporary markings” may also be applied on at least one of the two surfaces of the lens, indicating positions of control points (reference points) on the lens, such as a control point for far-vision, a control point for near-vision, a prism reference point and a fitting cross for instance. The prism reference point PRP is considered here at the midpoint of the straight segment which connects the micro-markings. If the temporary markings are absent or have been erased, it is always possible for a skilled person to position the control points on the lens by using a mounting chart and the permanent micro-markings. Similarly, on a semi-finished lens blank, standard ISO 10322-2 requires micro-markings to be applied. The centre of the aspherical surface of a semi-finished lens blank can therefore be determined as well as a referential as described above.

FIG. 3 shows field vision zones of an ophthalmic progressive addition lens 30 where said lens comprises a far vision (distant vision) zone 32 located in the upper part of the lens, a near vision zone 36 located in the lower part of the lens and an intermediate zone 34 situated between the far vision zone 32 and the near vision zone 36. The meridian line is referred as 38.

A plurality of criteria has been defined in the scope of the present invention and there definitions are illustrated by FIGS. 4 to 13.

In the background of FIGS. 4 to 11, the acuity loss contour plot of a same example of an ophthalmic progressive addition lens is represented.

In the background of FIG. 12, the module of resulting astigmatism contour plot of the same example of an ophthalmic progressive addition lens is represented.

In the background of FIG. 13, the norm of the gradient of resulting astigmatism contour plot of the same example of an ophthalmic progressive addition lens is represented.

The acuity loss contour shows the variations over the (α, β) domain of the acuity loss value ACU(α, β); the acuity loss value is expressed in log MAR.

The acuity loss value ACU(α, β) is defined according to following equation:

ACU(α,β)=−log(AC %(α,β)/100);

AC %(α, β) is an acuity function defined as a function of both mean refractive power, PPO(α, β), and module of resulting astigmatism, ASR(α, β); where:

• • one defines a mean refractive power difference function, P(α, β), where:

P(α,β)=PPO(α,β)−PPO(α,β_α_mer);

• • β_α_mer being the value of the azimuth angle β on the meridian line, ML(α, β), at the lowering angle α;
  • if P(α, β)≥0, AC %(α, β) is defined according to following equation:

AC %(α,β)={100−63×P(α,β)−44.3×ASR(α,β)+7.2×P(α,β)²+19.5×P(α,β)×ASR(α,β)+ASR(α,β)²}

• • if P(α, β)<0, AC %(α, β) is defined according to following equation:

AC %(α,β)=100−44.3×ASR(α,β)+ASR(α,β)².

Bibliographical reference of such an acuity loss definition can be found in following document: Fauquier, C., et al. “Influence of combined power error and astigmatism on visual acuity.” Vision Science and Its Applications, OSA Technical Digest Series. Washington, D.C.: Optical Society of America (1995): 151-4.

Acuity loss values ACU(α, β) of the example lens are plotted in the background of FIGS. 4 to 11 and curves indicates iso-acuity loss values where there is an increment of 0.1 log MAR between neighbouring curves of different acuity loss values. On all these figures, a circle, referred as CIR, is represented; said circle is centered on (α, β)=(12,0) and its radius is equal to 35 degree. Said circle represent the angular zone within which the criteria of the invention are defined.

FIG. 4 shows how to calculate criterion LAcuSub85(0.1); LAcuSub85(0.1) is the angular extent (in deg²) of the zone (in grey on the figure) between the two central neighbouring curves of acuity loss equal to 0.1 log MAR, said angular extent being calculated inside the circle CIR, and for lowering angle α more than α85% (i.e. for α≥α85%), where α85% is defined as the lowering angle where 85% of the prescribed addition is perceived by the wearer on the meridian line. The lowering angle of the meridian line where 85% of the prescribed addition is perceived by the wearer is defined in the frame of the present invention as being the angle lowering α where the mean refractive power, PPO(α85%), fulfills following equation:

PPO(α85%)=PPO(FVGD)+0.85×ADD_p,

and where PPO(FVGD) is the mean refractive power according to the far-vision gaze direction, FVGD.

Similar definition is used for “a lowering angle of the meridian line where 15% of the prescribed addition is perceived by the wearer” which corresponds to the lowering angle α where the mean refractive power, PPO(α15%), fulfills following equation:

PPO(α15%)=PPO(FVGD)+0.15×ADD_p.

FIG. 5 shows how to calculate criterion LAcuSub85(0.2); LAcuSub85(0.2) is the angular extent (in deg²) of the zone (in grey on the figure) between the two central neighbouring curves of acuity loss equal to 0.2 log MAR, said angular extent being calculated inside the circle CIR, and for lowering angle α more than α85% (i.e. for α≥α85%).

FIG. 6 shows how to calculate criterion LAcuAlpha85(0.1); LAcuAlpha85(0.1) is the acuity width (in deg) at α85% between the two central neighbouring curves of acuity loss equal to 0.1 log MAR; it is equal to β+(ACU(α85%, β)=0.1)−β−(ACU(α85%, β)=0.1), where β+ is greater than β_α_mer(α85%) and β− is less than β_α_mer(α85%).

FIG. 7 shows how to calculate criterion LAcuAlpha85(0.2); LAcuAlpha85(0.2) is the acuity width (in deg) at α85% between the two central neighbouring curves of acuity loss equal to 0.2 log MAR; it is equal to β+(ACU(α85%, β)=0.2)−β−(ACU(α85%, β)=0.2), where β+ is greater than β_α_mer(α85%) and β− is less than β_α_mer(α85%).

FIG. 8 shows how to calculate criterion LAcuSubFC(0.1); LAcuSubFC(0.1) is the angular extent (in deg²) of the zone (in grey on the figure) between the two central neighbouring curves of acuity loss equal to 0.1 log MAR, said angular extent being calculated inside the circle CIR, and for a more than α_FC (i.e. for α≥α_FC).

FIG. 9 shows how to calculate criterion LAcuSubFC(0.2); LAcuSubFC(0.2) is the angular extent (in deg²) of the zone (in grey on the figure) between the two central neighbouring curves of acuity loss equal to 0.2 log MAR, said angular extent being calculated inside the circle CIR, and for a more than α_FC (i.e. for α≥α_FC).

FIG. 10 shows how to calculate criterion LAcuDomain(0.1); LAcuDomain(0.1) is the angular extent (in deg²) of the zone (in grey on the figure) between the two central neighbouring curves of acuity loss equal to 0.1 log MAR, said angular extent being calculated inside the whole circle CIR.

FIG. 11 shows how to calculate criterion LAcuDomain(0.2); LAcuDomain(0.2) is the angular extent (in deg²) of the zone (in grey on the figure) between the two central neighbouring curves of acuity loss equal to 0.2 log MAR, said angular extent being calculated inside the whole circle CIR.

FIG. 12 shows how to calculate criterion PeaksMean; the module of resulting astigmatism values of the example lens are plotted in the background of FIG. 12 and curves indicates iso-module of resulting astigmatism values where there is an increment of 0.25 Diopter between neighbouring curves of different module of resulting astigmatism values. Previously defined Circle, CIR, is represented; PeaksMean is the mean maximum module of resulting astigmatism (in Diopter) which is equal to [ASR_max(α_L, β_L)+ASR_max(α_R, β_R)]/2, where ASR_max(α_L, β_L) is the maximum module of resulting astigmatism on a side (left side) of the meridian line, and ASR_max(α_R, β_R) is the maximum module of resulting astigmatism on the other side (right side) of the meridian line that are both determined inside the circle, CIR.

FIG. 13 shows how to calculate criterion AsrGradMax; the norm of the gradient of resulting astigmatism values of the example lens are plotted in the background of FIG. 13 and curves indicates iso-norm of the gradient of resulting astigmatism values where there is an increment of 0.05 Diopter between neighbouring curves of different norm of the gradient of resulting astigmatism values. AsrGradMax is defined as the maximum value of the norm of the gradient of resulting astigmatism, ASR(α, β), expressed in Diopter per degree, calculated inside the circle, CIR. The zone where said maximum value of the norm of the gradient of resulting astigmatism appears on FIG. 13 is indicated as a small circle for a about +15 degree.

Gradient of resulting astigmatism is a vector V which components are following:

$V_{\alpha }=\frac{\partial \mathrm{ASR}}{\partial \alpha }$ $V_{\beta }=\frac{\partial \mathrm{ASR}}{\partial \beta }$

Its norm is given by following equation:

∥V∥=√{square root over (V_α²+V_β²)}

According to an example, one determinates the gradient of resulting astigmatism using a finite difference method;According to an example:

$V_{\alpha }\approx \frac{\mathrm{ASR}\left(\alpha +\varepsilon ,\beta \right)-\mathrm{ASR}\left(\alpha -\varepsilon ,\beta \right)}{2\varepsilon }$ $V_{\beta }\approx \frac{\mathrm{ASR}\left(\alpha ,\beta +\varepsilon \right)-\mathrm{ASR}\left(\alpha ,\beta -\varepsilon \right)}{2\varepsilon }$

According to an example, ε=0.1 deg.Circle, referred as CIR, and centered on (α, β)=(12,0) with a radius is equal to 35 degree is called “Domain”. AsrGradMax can be defined according to following equation:

AsrGradMax=Max{∥V(α,β)∥;(α,β)ϵDomain}

FIG. 14 shows the variation of object proximity ProxO as a function of the lowering angle α used to define the ergorama in view of U.S. Pat. No. 6,318,859.

The ergorama used in the frame of the present invention is defined thanks to following data, where object proximity values are given for lowering angles α:

Alpha ProxO
[deg] [D]
−50   0
−40   0
−30   0
−20   0
−10   0
0     0
10    1.65
20    2.54
30    2.78
40    2.93
50    2.98

EXAMPLES

FIGS. 15 to 18 give optical characteristics of an ophthalmic progressive addition lens according to the prior art, hereafter referred as “PA_lens”.

FIGS. 19 to 22 give optical characteristics of an ophthalmic progressive addition lens according to the invention, hereafter referred as “INV_lens”.

Said both ophthalmic progressive addition lenses have been designed so as to fulfil following prescribed features:

prescribed sphere SPH_p=0 Diopter

prescribed astigmatism value CYL_p=0 Diopter

prescribed axis AXIS_p=0°

prescribed addition ADD_p=2 Diopter

FIGS. 15 and 19 represent the mean refractive power repartition profile, PPO, as a function of the lowering angle α, along the meridian line, for respectively the prior art ophthalmic progressive addition lens and the ophthalmic progressive addition lens according to the present invention. Lowering angles corresponding to α85% and to α15% are indicated.

FIGS. 16 and 20 represent the mean refractive power repartition, PPO, over the (α, β) domain, for respectively the prior art ophthalmic progressive addition lens and the ophthalmic progressive addition lens according to the present invention. Curves indicates iso-mean refractive power values where there is an increment of 0.25 Diopter between neighbouring curves of different module of resulting astigmatism values.

FIGS. 17 and 21 represent respectively the module of resulting astigmatism repartition, ASR, over the (α, β) domain, for respectively the prior art ophthalmic progressive addition lens and the ophthalmic progressive addition lens according to the present invention. Curves indicates iso-module of resulting astigmatism values where there is an increment of 0.25 Diopter between neighbouring curves of different module of resulting astigmatism values.

FIGS. 18 and 22 represent respectively the acuity loss value repartition ACU, over the (α, β) domain, for respectively the prior art ophthalmic progressive addition lens and the ophthalmic progressive addition lens according to the present invention. Curves indicates iso-acuity loss values where there is an increment of 0.1 log MAR between neighbouring curves of different module of resulting astigmatism values.

Here above defined acuity criteria have been calculated for the said both ophthalmic progressive addition lenses. Results are reported here bellow.

	Lens	PA_lens	INV_lens
	AcuityCriterion1	431	520
	AcuityCriterion2	1015	1190
	AcuityCriterion3	37	40
	AcuityCriterion4	58	61
	AcuityCriterion5	84	90
	AcuityCriterion6	117	122

The inventors have done tests that demonstrate that the chosen threshold value of AcuityCriterion1, and optionally the chosen threshold values of AcuityCriterion2 and/or AcuityCriterion3 and/or AcuityCriterion4 and/or AcuityCriterion5 and/or AcuityCriterion6, is (are) suitable for providing to an emmetropic and presbyopic wearer an ophthalmic progressive addition lens where the wearer's visual comfort is enhanced in view of known prior art ophthalmic progressive addition lens.

Claims

1: An ophthalmic progressive addition lens for an emmetropic and presbyopic wearer which has a prescribed far vision mean refractive power greater than minus 1 Diopter and less than plus 1 Diopter and a non nil prescribed addition, ADDp, said lens having a mean refractive power, PPO(α, β), a module of resulting astigmatism, ASR(α, β), an acuity loss value ACU(α, β), where said (α, β) functions are determined in as-worn conditions of the lens by the wearer, and a first acuity criterion, AcuityCriterion1 which fulfils following requirement: AcuityCriterion1≥435D2·deg2 and where:“D” refers to Diopter, “deg” to degree, AcuityCriterion1 is defined as a combination of PPO(α, β), ASR(α, β), ADDp, and ACU(α, β).

2: An ophthalmic progressive addition lens as claimed in claim 1, according to which said lens is further characterized by a meridian line, ML(α, β), a fitting cross, FC(αFC, βFC), said (α, β) functions being determined in as-worn conditions of the lens by the wearer for gaze directions (α, β) joining the center of rotation of the eye, CRE, and the lens, where α is a lowering angle in degree and β is an azimuth angle in degree and wherein: the acuity loss value ACU(α, β) is expressed in log MAR and defined according to following equation: ACU(α,β)=−log(AC %(α,β)/100), where:AC %(α, β)=100−63×P(α, β)−44.3×ASR(α, β)+7.2×P(α, β)2+19.5×P(α, β)×ASR(α, β)+ASR(α, β)2; when P(α, β)≥0; andAC %(α, β)=100−44.3×ASR(α, β)+ASR(α, β)2; when P(α, β)<0;P(α, β)=PPO(α, β)−PPO(α,β_α_mer);β_α_mer is the value of the azimuth angle β on the meridian line, ML(α, β), at the lowering angle α;and where AcuityCriterion1=Numerator1/Denominator;Numerator1=LAcuSub85(0.1)×LAcuAlpha85(0.1)×ADDp4;Denominator=AsrGradMax×PeaksMean×PVL2;LAcuSub85(0.1) is the angular extent (in deg2) of the zone where ACU(α, β)≤0.1 log MAR, inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees, and where α≥α85%, α85% being the lowering angle where 85% of the prescribed addition is perceived by the wearer on the meridian line;LAcuAlpha85(0.1) is the acuity width (in deg) at α85% between two iso-acuity loss lines corresponding to 0.1 log MAR and is equal to β+ (ACU(α85%, β)=0.1)−β−(ACU(α85%, β)=0.1), where β+ is greater than β_α_mer(α85%) and β− is less than β_α_mer(α85%);PVL is the power variation length is expressed in deg and defined as being equal to (α85%−α15%), α15% being the lowering angle where 15% of the prescribed addition is perceived by the wearer on the meridian line;AsrGradMax is the maximum value of the norm of the gradient of resulting astigmatism, ASR(α, β), expressed in Diopter per degree, calculated inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees;PeaksMean is the mean maximum module of resulting astigmatism (in Diopter) which is equal to [ASRmax(αL, βL)+ASRmax(αR, βR)]/2, where ASRmax(αL, βL) is the maximum module of resulting astigmatism on a side (left side) of the meridian line, and ASRmax(αR, βR) is the maximum module of resulting astigmatism on the other side (right side) of the meridian line that are both determined inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees.

3: An ophthalmic progressive addition lens as claimed in claim 1, according to which a second acuity criterion, AcuityCriterion2, fulfils following requirement: AcuityCriterion2≥1100 D2·deg2, where:AcuityCriterion2=Numerator2Denominator;Numerator2=LAcuSub85(0.2)×LAcuAlpha85(0.2)×ADDp4;LAcuSub85(0.2) is the angular extent (in deg2) of the zone where ACU(α, β)≤0.2 log MAR, inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees, and where α≥α85%;LAcuAlpha85(0.2) is the acuity width (in deg) at α85% between two iso-acuity loss lines corresponding to 0.2 log MAR and is equal to β+(ACU(α85%, β)=0.2)−β−(ACU(α85%, β)=0.2), where β+ is greater than β_α_mer(α85%) and β− is less than β_α_mer(α85%).

4: An ophthalmic progressive addition lens as claimed in claim 1, according to which a third acuity criterion, AcuityCriterion3, fulfils following requirement: AcuityCriterion3≥37.4D·deg, where:AcuityCriterion3=Numerator3 Denominator;Numerator3=LAcuSubFC(0.1)×ADDp3;LAcuSubFC(0.1) is the angular extent (in deg2) of the zone where ACU(α, β)≤0.1 log MAR, inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees, and where α≥αFC.

5: An ophthalmic progressive addition lens as claimed in claim 1, according to which a fourth acuity criterion, AcuityCriterion4, fulfils following requirement: AcuityCriterion4≥58.4D·deg, where:AcuityCriterion4=Numerator4 Denominator;Numerator4=LAcuSubFC(0.2)×ADDp3;LAcuSubFC(0.2) is the angular extent (in deg2) of the zone where ACU(α, β)≤0.2 log MAR, inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees, and where α≥αFC.

6: An ophthalmic progressive addition lens as claimed in claim 1, according to which a fifth acuity criterion, AcuityCriterion5, fulfils following requirement: AcuityCriterion5≥85 D·deg, where:AcuityCriterion5=Numerator5/Denominator;Numerator5=LAcuDomain(0.1)×ADDp3;LAcuDomain(0.1) is the angular extent (in deg2) of the zone where ACU(α, β)≤0.1 log MAR, inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees.

7: An ophthalmic progressive addition lens as claimed in claim 1, according to which a sixth acuity criterion, AcuityCriterion6, fulfils following requirement: AcuityCriterion6≥117.5 D·deg, where:AcuityCriterion6=Numerator6/Denominator;Numerator6=LAcuDomain(0.2)×ADDp3;LAcuDomain(0.2) is the angular extent (in deg2) of the zone where ACU(α, β)≤0.2 log MAR, inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees.

8: A method implemented by computer means for providing an ophthalmic progressive addition lens to an emmetropic and presbyopic wearer having a prescribed far vision mean refractive power greater than minus 1 Diopter and less than plus 1 Diopter and a non nil prescribed addition, ADDp, comprising the step of calculating a mean refractive power repartition, PPO(α, β), a module of resulting astigmatism repartition, ASR(α, β), an acuity loss value repartition ACU(α, β), where said (α, β) functions are calculated in as-worn conditions of the lens by the wearer, so as to fulfil following requirement of a first acuity criterion, AcuityCriterion1: AcuityCriterion1≥435D2·deg2;“D” refers to Diopter, “deg” to degree, AcuityCriterion1 is defined as a combination of PPO(α, β), ASR(α, β), ADDp, and ACU(α, β).

9: The method for providing an ophthalmic progressive addition lens as claimed in claim 8, further comprising following steps: Calculating or defining a meridian line, ML(α, β),Calculating or defining a fitting cross, FC(αFC, βFC),Calculating the mean refractive power, PPO(α, β), and the module of resulting astigmatism, ASR(α, β), determined in as-worn conditions of the lens by the wearer for gaze directions (α, β) joining the center of rotation of the eye, CRE, and the lens, where α is a lowering angle in degree and β is an azimuth angle in degree, an acuity loss value ACU(α, β) is expressed in log MAR and defined according to following equation: ACU(α,β)=−log(AC %(α,β)/100), where:AC %(α, β)=100−63×P(α, β)−44.3×ASR(α, β)+7.2×P(α, β)2+19.5×P(α, β)×ASR(α, β)+ASR(α, β)2; when P(α, β)≥0; andAC %(α, β)=100−44.3×ASR(α, β)+ASR(α, β)2; when P(α, β)<0;P(α, β)=PPO(α, β)−PPO(α,β_α_mer);β_α_mer is the value of the azimuth angle β on the meridian line, ML(α, β), at the lowering angle α;and where AcuityCriterion1=Numerator1/Denominator; Numerator1=LAcuSub85(0.1)×LAcuAlpha85(0.1)×ADDp4;Denominator=AsrGradMax×PeaksMean×PVL2;LAcuSub85(0.1) is the angular extent (in deg2) of the zone where ACU(α, β)≤0.1 log MAR, inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees, and where α≥α85%, α85% being the lowering angle where 85% of the prescribed addition is perceived by the wearer on the meridian line;LAcuAlpha85(0.1) is the acuity width (in deg) at α85% between two iso-acuity loss lines corresponding to 0.1 log MAR and is equal to: β+(ACU(α85β)−β−(ACU(α85%, β)=0.1), where β+ is greater than β_α_mer(α85%) and β− is less than β_α_mer(α85%);PVL is the power variation length is expressed in deg and defined as being equal to (α85%−α15%), α15% being the lowering angle where 15% of the prescribed addition is perceived by the wearer on the meridian line;AsrGradMax is the maximum value of the noun of the gradient of resulting astigmatism, ASR(α, β), expressed in Diopter per degree, calculated inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees;PeaksMean is the mean maximum module of resulting astigmatism (in Diopter) which is equal to [ASRmax(αL, βL)+ASRmax(αR, βR)]/2, where ASRmax(αL, βL) is the maximum module of resulting astigmatism on a side (left side) of the meridian line, and ASRmax(αR, βR) is the maximum module of resulting astigmatism on the other side (right side) of the meridian line that are both determined inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees.

10: The method for providing an ophthalmic progressive addition lens as claimed claim 8, according to which one calculates the lens so as to fulfil following requirement of a second acuity criterion, AcuityCriterion2: AcuityCriterion2≥1100 D2·deg2, where:AcuityCriterion2=Numerator2/Denominator;Numerator2=LAcuSub85(0.2)×LAcuAlpha85(0.2)×ADDp4;LAcuSub85(0.2) is the angular extent (in deg2) of the zone where ACU(α, β)≤0.2 log MAR, inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees, and where α≥α85%;LAcuAlpha85(0.2) is the acuity width (in deg) at α85% between two iso-acuity loss lines corresponding to 0.2 log MAR and is equal to β+(ACU(α85%, β)=0.2)−β−(ACU(α85%, β)=0.2), where β+ is greater than α_α_mer(α85%) and β− is less than β_α_mer(α85%).

11: The method for providing an ophthalmic progressive addition lens as claimed in claim 8, according to which one calculates the lens so as to fulfil following requirement of a third acuity criterion, AcuityCriterion3: AcuityCriterion3≥37.4 D·deg, where:AcuityCriterion3=Numerator3/Denominator;Numerator3=LAcuSubFC(0.1)×ADDp3;LAcuSubFC(0.1) is the angular extent (in deg2) of the zone where ACU(α, β)≤0.1 log MAR, inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees, and where α≥αFC.

12: The method for providing an ophthalmic progressive addition lens as claimed in claim 8, according to which one calculates the lens so as to fulfil following requirement of a fourth acuity criterion, AcuityCriterion4: AcuityCriterion4≥58.4 D·deg, where:AcuityCriterion4=Numerator4 Denominator;Numerator4=LAcuSubFC(0.2)×ADDp3;LAcuSubFC(0.2) is the angular extent (in deg2) of the zone where ACU(α, β)≤0.2 log MAR, inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees, and where α≥αFC.

13: The method for providing an ophthalmic progressive addition lens as claimed in claim 8, according to which one calculates the lens so as to fulfil following requirement of a fifth acuity criterion, AcuityCriterion5: AcuityCriterion5≥85 D·deg, where:AcuityCriterion5=Numerator5 Denominator;Numerator5=LAcuDomain(0.1)×ADDp;LAcuDomain(0.1) is the angular extent (in deg2) of the zone where ACU(α, β)≤0.1 log MAR, inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees.

14: The method for providing an ophthalmic progressive addition lens as claimed in claim 8, according to which one calculates the lens so as to fulfil following requirement of a sixth acuity criterion, AcuityCriterion6: AcuityCriterion6≥117.5 D·deg, where:AcuityCriterion6=Numerator6/Denominator;Numerator6=LAcuDomain(0.2)×ADDp3;LAcuDomain(0.2) is the angular extent (in deg2) of the zone where ACU(α, β)≤0.2 log MAR, inside a circle, CIR, centered on (α, β)=(12,0), which radius is 35 degrees.

15: The method for providing an ophthalmic progressive addition lens as claimed in claim 8, according to which the method comprises an optimization routine where at least a target is chosen within requirement of an acuity criterion chosen in the list consisting of AcuityCriterion1, AcuityCriterion2, AcuityCriterion3, AcuityCriterion4, AcuityCriterion5, AcuityCriterion6.