IP Library › Granted Patent US 11,271,544
Granted Patent B2
US 11,271,544 · App. 16/783,202 · Granted Mar 8, 2022

Multiplexer, high-frequency front end circuit, and communication device

Inventors: Ryo Nakagawa (Nagaokakyo, JP); Shou Nagatomo (Nagaokakyo, JP); Hideki Iwamoto (Nagaokakyo, JP); Tsutomu Takai (Nagaokakyo, JP)
Assignee: MURATA MANUFACTURING CO., LTD.
H03H9/25H03H9/02559H03H9/02574H03H9/14502H03H9/6406H03H9/6483H03H9/725
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Quick Facts
Patent No.
US 11,271,544
App. No.
16/783,202
Granted
Mar 8, 2022
Kind
B2
Abstract

A multiplexer includes N acoustic wave filters each including one end connected in common and having a different pass band, in which when the N acoustic wave filters are in order from a side of a lower frequency of the pass band, at least one n-th acoustic wave filter among the N acoustic wave filters excluding an acoustic wave filter having the highest frequency of the pass band includes one or more acoustic wave resonators including a support substrate, a silicon nitride film laminated on the support substrate, a silicon oxide film laminated on the silicon nitride film, a piezoelectric body laminated on the silicon oxide film, and an IDT electrode provided on the piezoelectric body. All acoustic wave filters having a pass band in a higher frequency than a frequency of a pass band of the n-th acoustic wave filter satisfy f h1_t (n) >f u (m) or f h1_t (n) <f l (m) .

Claims (1746)

1. A multiplexer comprising:

N acoustic wave filters each including one end connected in common and having different pass bands, where, N is an integer equal to or greater than 2; wherein

when the N acoustic wave filters include a first acoustic wave filter, a second acoustic wave filter, . . . , and an N-th acoustic wave filter in order from a side of a lower frequency of the pass band, at least one acoustic wave filter n, where 1≤n<N, among the N acoustic wave filters excluding an acoustic wave filter having the highest frequency of the pass band includes one or more acoustic wave resonators;

a t-th acoustic wave resonator among the one or more acoustic wave resonators includes:

a support substrate having Euler angles (φ Si , θ Si , ψ Si ) and made of silicon;

a silicon nitride film on the support substrate;

a silicon oxide film on the silicon nitride film;

a piezoelectric body on the silicon oxide film, having Euler angles (φ LT in a range of about 0° 5 , θ LT , yLT in a range of about 0° 15 ), and made of lithium tantalate; and

an interdigital transducer (IDT) electrode on the piezoelectric body;

when a wavelength determined by an electrode finger pitch of the IDT electrode is denoted as Δ in the t-th acoustic wave resonator, a thickness normalized by the wavelength λ is denoted as a wavelength normalized thickness, when setting values of T LT as a wavelength normalized thickness of the piezoelectric body, θ LT as an Euler angle of the piezoelectric body, T S as a wavelength normalized thickness of the silicon oxide film, T N as a wavelength normalized thickness of the silicon nitride film, T E as a wavelength normalized thickness of the IDT electrode converted to a thickness of aluminum, obtained by a product of a value obtained by dividing a density of the IDT electrode by a density of aluminum and a wavelength normalized thickness of the IDT electrode, ψ Si , as a propagation orientation in the support substrate, and T Si as a wavelength normalized thickness of the support substrate, at least one of frequencies f hs_t (n) of first, second, and third higher-order modes, where, s is 1, 2, or 3, and a case in which s is 1 indicates a frequency of the first higher-order mode, a case in which s is 2 indicates a frequency of the second higher-order mode, and a case in which s is 3 indicates a frequency of the third higher-order mode, determined by an expression (1) and an expression (2) below determined by the T LT , the θ LT , the T S , the T N , the T E , the ψ Si , and the T Si , and all m-th acoustic wave filters, wherein n<m≤N, each having a pass band of a higher frequency than a frequency of a pass band of the n-th acoustic wave filter satisfy an expression (3) or an expression (4) below:

V

=

a

T

(

3

)

⁡

(

(

T

+

c

)

3

+

b

(

3

)

)

+

a

T

(

2

)

⁡

(

(

T

+

c

)

2

+

b

(

2

)

)

+

a

(

1

)

⁡

(

T

+

c

)

+

a

(

2

)

⁡

(

(

T

S

+

c

)

2

+

b

(

2

)

)

+

a

T

S

(

1

)

⁡

(

T

S

+

c

T

)

+

a

(

2

)

⁡

(

(

T

N

+

c

)

2

+

b

(

2

)

)

+

a

T

(

1

)

⁡

(

T

N

+

c

T

)

+

a

T

E

(

1

)

⁡

(

T

E

+

c

T

E

)

+

a

ψ

(

5

)

⁡

(

(

ψ

Si

+

c

ψ

)

5

+

b

(

5

)

)

+

a

ψ

(

4

)

⁡

(

(

ψ

Si

+

c

ψ

Si

)

4

+

b

ψ

(

4

)

)

+

a

ψ

Si

(

3

)

⁡

(

(

ψ

Si

+

c

ψ

Si

)

3

+

b

ψ

Si

(

3

)

)

+

a

ψ

Si

(

2

)

⁡

(

(

ψ

Si

+

c

ψ

)

2

+

b

ψ

Si

(

2

)

)

+

a

ψ

Si

(

1

)

⁡

(

ψ

Si

+

c

ψ

Si

)

+

e

;

Expression

⁢

⁢

(

1

)

f

h

s

⁢

_

⁢

⁢

t

(

n

)

=

V

h

s

⁢

_

⁢

⁢

t

λ

t

(

n

)

,

(

s

=

1

,

2

,

3

)

;

Expression

⁢

⁢

(

2

)

f

hs

⁢

⁢

_

⁢

⁢

t

(

n

)

>

f

u

(

m

)

;

Expression

⁢

⁢

(

3

)

f

hs

⁢

⁢

_

⁢

⁢

t

(

n

)

<

f

l

(

m

)

;

Expression

⁢

⁢

(

4

)

the f hs_t (n) represents a frequency of a higher-order mode corresponding to the s in the t-th acoustic wave resonator included in n-th the acoustic wave filter;

the λ t (n) is a wavelength determined by the electrode finger pitch of the IDT electrode in the t-th acoustic wave resonator included in the n-th acoustic wave filter;

the f u (m) is a frequency of a high band side end portion of the pass band in each of the m-th acoustic wave filters;

the f l (m) is a frequency of a low band side end portion of the pass band in each of the m-th acoustic wave filters; and

each coefficient in the expression (1) is each value shown in Table 1, Table 2, or Table 3 indicated below for each value of the s and each crystal orientation of the support substrate:

TABLE 1

s = 1,

First

Higher-

Order

Mode

Si(100)

Si(110)

Si(111)

a TLT (3)

0

0

0

a TLT (2)

0

0

0

a TLT (1)

−128.109974

−84.392576

−78.4352

b TLT (3)

0

0

0

b TLT (2)

0

0

0

c TLT

−0.2492038

−0.247604

−0.24838

a TS (2)

0

0

0

a TS (1)

−109.6889

−182.2936559

−485.867

b TS (2)

0

0

0

c TS

−0.249363

−0.2498958

−0.24942

a TN (2)

−337.59528

−198.4171235

−264.804

a TN (1)

−109.08389

38.137636

−20.3216

b TN (2)

−0.0262274

−0.04671597

−0.04389

c TN

−0.29617834

0.369166

−0.34988

a TE (1)

175.4682

13.0363945

0

c TE

−0.14826

−0.14979166

0

a ψSi (5)

0

0

0

a ψSi (4)

0

0.000489723

0.000503

a ψSi (3)

0.0236358

−5.09E−05

0.006871

a ψSi (2)

−0.0357088

−1.01733189

−0.80395

a ψSi (1)

−34.8157175

0

−5.57553

b ψSi (5)

0

0

0

b ψSi (4)

0

−2150682.513

−352545

b ψSi (3)

0

−21460.18941

2095.94

b ψSi (2)

−288.415605

−36.8125

−33.3025

c ψSi

−22.5

−36.8125

−33.3025

e

5251.687898

5092.365583

4851.236

TABLE 2

s = 2,

Second

Higher-

Order

Mode

Si(100)

Si(110)

Si(111)

a TLT (3)

0

0

0

a TLT (2)

2285.602094

3496.38329

−2357.61

a TLT (1)

−538.88053

−1081.86178

−1308.55

b TLT (3)

0

0

0

b TLT (2)

−0.0016565

−0.001741462

−0.00166

c TLT

−0.251442

−0.2501547

−0.2497

a TS (2)

−3421.09725

−4927.3017

−3633.11

a TS (1)

−1054.253

−992.33158

−1006.69

b TS (2)

−0.0016565

−0.2551083

−0.00166

c TS

−0.2514423

0.2551

−0.25019

a TN (2)

1042.56084

−423.87007

−135.325

a TN (1)

159.11219

80.7948

−106.73

b TN (2)

−0.02613905

−0.05219411

−0.0486

c TN

−0.2961538

−0.36996

−0.39884

a TE (1)

−171.153846

−637.391944

−585.696

c TE

0.15

−0.151238

−0.14932

a ψSi (5)

0

0

0

a ψSi (4)

0

−0.00098215

−0.00016

a ψSi (3)

−0.0038938

−0.002109232

−0.00037

a ψSi (2)

−0.00306409

2.25463

0.224668

a ψSi (1)

2.8538478

23.6872514

1.243381

b ψSi (5)

0

0

0

b ψSi (4)

0

−2959279.229

−399785

b ψSi (3)

234.60436

−21928.45828

5.712562

b ψSi (2)

−289.82063

−1407.041187

−535.077

c ψSi

22.78846

−39.1640886

−29.9806

e

5282.98076

5338.606811

5411.395

TABLE 3

s = 3,

Third

Higher-

Order

Mode

Si(100)

Si(110)

Si(111)

a TLT (3)

0

0

0

a TLT (2)

0

0

3595.754

a TLT (1)

−782.3425

−1001.237815

−592.246

b TLT (3)

0

0

0

b TLT (2)

0

0

−0.00164

c TLT

−0.254819

−0.2578947

−0.25367

a TS (2)

−14897.59116

0

0

a TS (1)

−599.8312

−686.9212563

−438.155

b TS (2)

−0.00162005

0

0

c TS

−0.25682

−0.25546558

−0.25562

a TN (2)

0

0

0

a TN (1)

0

125.557557

15.72663

b TN (2)

0

0

0

c TN

0

−0.349392713

−0.40872

a TE (1)

−154.8823

−764.8758717

−290.54

c TE

−0.14819277

−0.15303646

−0.15149

a ψSi (5)

0

0

0

a ψSi (4)

0

0

−0.00073

a ψSi (3)

0.010467682

−0.000286554

−0.00318

a ψSi (2)

−0.196913569

0.67197739

0.969126

a ψSi (1)

−0.3019959

0.197549

0.359421

b ψSi (5)

0

0

0

b ψSi (4)

0

−0.000204665

0

b ψSi (3)

0

−14837.92017

670.2052

b ψSi (2)

−240.3687037

−1590.306348

−525.572

c ψSi

24.4578313

−41.9028

−31.1239

e

5730.906036

5574.008097

5675.837.

2. The multiplexer according to claim 1 , wherein the wavelength normalized thickness T Si of the support substrate satisfies T Si >about 4.

3. The multiplexer according to claim 2 , wherein T Si >about 10 is satisfied.

4. The multiplexer according to claim 3 , wherein T Si >about 20 is satisfied.

5. The multiplexer according to claim 1 , wherein the wavelength normalized thickness of the piezoelectric body is equal to or less than about 3.5λ.

6. The multiplexer according to claim 5 , wherein the wavelength normalized thickness of the piezoelectric body is equal to or less than about 2.5λ.

7. The multiplexer according to claim 5 , wherein the wavelength normalized thickness of the piezoelectric body is equal to or less than about 1.5λ.

8. The multiplexer according to claim 5 , wherein the wavelength normalized thickness of the piezoelectric body is equal to or less than about 0.5λ.

9. The multiplexer according to claim 1 , further comprising:

an antenna terminal to which one ends of the plurality of acoustic wave filters are connected in common; wherein

the multiplexer is a composite filter in which three or more acoustic wave filters are connected in common on a side of the antenna terminal.

10. The multiplexer according to claim 9 , wherein the multiplexer is a composite filter device for carrier aggregation.

11. The multiplexer according to claim 1 , wherein the values of the T LT , the θ LT , the T S , the T N , the T E , the ψ Si , and the T Si , are selected such that the frequencies f hs_t (n) of the first and second higher-order modes satisfy the expression (3) or the expression (4).

12. The multiplexer according to claim 1 , wherein the values of the T LT , the θ LT , the T S , the T N , the T E , the ψ Si , and the T Si , are selected such that the frequencies f hs_t (n) of the first and third higher-order modes satisfy the expression (3) or the expression (4).

13. The multiplexer according to claim 1 , wherein the values of the T LT , the θ LT , the T S , the T N , the T E , the ψ Si , and the T Si , are selected such that the frequencies f hs_t (n) of the second and third higher-order modes satisfy the expression (3) or the expression (4).

14. The multiplexer according to claim 1 , wherein the values of the T LT , the θ LT , the T S , the T N , the T E , the ψ Si , and the T Si , are selected such that all the frequencies f hs_t (n) of the first, second, and third higher-order modes satisfy the expression (3) or the expression (4).

15. The multiplexer according to claim 1 , the multiplexer further comprising:

an antenna terminal to which one ends of the plurality of acoustic wave filters are connected in common; wherein

the acoustic wave resonator satisfying the expression (3) or the expression (4) is an acoustic wave resonator of the one or more acoustic wave resonators which is closest to the antenna terminal.

16. The multiplexer according to claim 1 , wherein all of the one or more acoustic wave resonators are each the acoustic wave resonator satisfying the expression (3) or the expression (4).

17. The multiplexer according to claim 1 , wherein the multiplexer is a duplexer.

18. The multiplexer according to claim 1 , wherein the acoustic wave filter including the one or more acoustic wave resonators is a ladder filter including a plurality of serial arm resonators and a plurality of parallel arm resonators.

19. A multiplexer comprising:

N acoustic wave filters each including one end connected in common and having different pass bands, where, N is an integer equal to or greater than 2; wherein

when the N acoustic wave filters include a first acoustic wave filter, a second acoustic wave filter, and . . . , an N-th acoustic wave filter in order from a side of a lower frequency of the pass band, at least one n-th acoustic wave filter, wherein 1≤n<N, among the N acoustic wave filters excluding an acoustic wave filter having the highest frequency of the pass band includes one or more acoustic wave resonators;

a t-th acoustic wave resonator among the one or more acoustic wave resonators includes:

a support substrate having Euler angles (φ Si , θ Si , ψ Si ) and made of silicon;

a silicon nitride film on the support substrate;

a silicon oxide film on the silicon nitride film;

a piezoelectric body on the silicon oxide film, having Euler angles (φ LT in a range of about 0°±5°, θ LT , ψ LT in a range of about 0°±15°), and made of lithium tantalate; and

an interdigital transducer (IDT) electrode on the piezoelectric body;

when a wavelength determined by an electrode finger pitch of the IDT electrode is denoted as λ in the t-th acoustic wave resonator, a thickness normalized by the wavelength λ is denoted as a wavelength normalized thickness, when setting values of T LT as a wavelength normalized thickness of the piezoelectric body, θ LT as an Euler angle of the piezoelectric body, T S as a wavelength normalized thickness of the silicon oxide film, T N as a wavelength normalized thickness of the silicon nitride film, T E as a wavelength normalized thickness of the IDT electrode converted to a thickness of aluminum, obtained by a product of a value obtained by dividing a density of the IDT electrode by a density of aluminum and a wavelength normalized thickness of the IDT electrode, ψ Si as a propagation orientation in the support substrate, and T Si as a wavelength normalized thickness of the support substrate, at least one of frequencies f hs_t (n) of first, second, and third higher-order modes, where s is 1, 2, or 3, and a case in which s is 1 indicates a frequency of the first higher-order mode, a case in which s is 2 indicates a frequency of the second higher-order mode, and a case in which s is 3 indicates a frequency of the third higher-order mode, determined by an expression (5) and an expression (2) below determined by the T LT , the θ LT , the T S , the T N , the T E , the ψ Si , and the T Si , and all m-th acoustic wave filters (n<m≤N) each having a pass band of a higher frequency than a frequency of a pass band of the n-th acoustic wave filter satisfy an expression (3) or an expression (4)

V

h

=

a

T

LT

(

2

)

⁡

(

(

T

LT

-

c

T

)

2

-

b

T

(

2

)

)

+

a

(

1

)

⁡

(

T

LT

-

c

T

)

+

a

(

2

)

⁡

(

(

T

S

-

c

T

S

)

2

-

b

T

(

2

)

)

+

a

T

S

(

1

)

⁡

(

T

S

-

c

T

)

+

a

T

N

(

3

)

⁡

(

(

T

N

-

c

T

N

)

3

-

b

T

N

(

3

)

)

+

a

T

N

(

2

)

⁡

(

(

T

N

-

c

T

N

)

2

-

b

T

N

(

2

)

)

+

a

T

N

(

1

)

⁡

(

T

N

-

c

T

N

)

+

a

T

E

(

1

)

⁡

(

T

E

-

c

T

E

)

+

a

ψ

Si

(

4

)

⁡

(

(

ψ

Si

-

c

ψ

Si

)

4

-

b

ψ

Si

(

4

)

)

+

a

ψ

Si

(

3

)

⁡

(

(

ψ

Si

-

c

ψ

Si

)

3

-

b

ψ

Si

(

3

)

)

+

a

ψ

Si

(

2

)

⁡

(

(

ψ

Si

-

c

ψ

)

2

-

b

ψ

(

2

)

)

+

a

ψ

(

1

)

⁡

(

ψ

Si

-

c

ψ

Si

)

+

a

θ

LT

(

1

)

⁡

(

θ

LT

-

c

θ

LT

)

+

d

T

LT

⁢

T

S

⁡

(

T

LT

-

c

T

LT

)

⁢

(

T

S

-

c

T

)

+

d

⁡

(

T

LT

-

c

LT

)

⁢

(

T

N

-

c

T

N

)

+

d

⁡

(

T

LT

-

c

T

LT

)

⁢

(

ψ

Si

-

c

ψ

Si

)

+

d

T

S

⁢

T

N

⁡

(

T

S

-

c

T

S

)

⁢

(

T

N

-

c

T

N

)

+

d

T

N

⁢

ψ

Si

⁡

(

T

N

-

c

T

N

)

⁢

(

ψ

Si

-

c

ψ

Si

)

+

d

T

⁢

θ

LT

⁡

(

T

N

-

c

T

N

)

⁢

(

θ

LT

-

c

θ

LT

)

+

d

T

⁢

ψ

Si

⁡

(

T

E

-

c

T

E

)

⁢

(

ψ

Si

-

c

ψ

Si

)

+

d

⁡

(

ψ

Si

-

c

ψ

Si

)

⁢

(

θ

LT

-

c

θ

LT

)

+

e

;

Expression

⁢

⁢

(

5

)

f

h

s

⁢

_

⁢

⁢

t

(

n

)

=

V

h

s

⁢

_

⁢

⁢

t

λ

t

(

n

)

,

(

s

=

1

,

2

,

3

)

;

Expression

⁢

⁢

(

2

)

f

hs

⁢

⁢

_

⁢

⁢

t

(

n

)

>

f

u

(

m

)

;

Expression

⁢

⁢

(

3

)

f

hs

⁢

⁢

_

⁢

⁢

t

(

n

)

<

f

l

(

m

)

;

Expression

⁢

⁢

(

3

)

the f hs_t (n) represents a frequency of a higher-order mode corresponding to the s in the t-th acoustic wave resonator included in the n-th acoustic wave filter;

the λ t (n) is a wavelength determined by the electrode finger pitch of the IDT electrode in the t-th acoustic wave resonator included in the n-th acoustic wave filter;

the f u (m) is a frequency of a high band side end portion of the pass band in each of the m-th acoustic wave filters;

the f l (m) is a frequency of a low band side end portion of the pass band in each of the m-th acoustic wave filters; and

each coefficient in the expression (5) is each value shown in Table 4, Table 5, or Table 6 below for each value of the s and each crystal orientation of the support substrate:

TABLE 4

s = 1,

First

Higher-

Order

Mode

Si(100)

Si(110)

Si(111)

a TLT (2)

0

0

0

a TLT (1)

0

0

0

b TLT (2)

0

0

0

c TLT

0

0

0

a TS (2)

0

0

0

a TS (1)

0

0

534.5188318

b TS (2)

0

0

0

c TS

0

0

0.249010293

a TN (3)

0

0

0

a TN (2)

0

0

0

a TN (1)

0

0

−36.51741324

b TN (3)

0

0

0

b TN (2)

0

0

0

c TN

0

0

0.35114806

a TE (1)

0

0

0

c TE

0

0

0

a ψSi (4)

0

0

0.000484609

a ψSi (3)

0.022075968

0

0.005818261

a ψSi (2)

−0.18782287

0.081701713

−0.805302371

a ψSi (1)

−33.85785847

10.57201342

−4.785681077

b ψSi (4)

0

0

351437.8188

b ψSi (3)

806.2400011

0

−1862.605341

b ψSi (2)

270.2635345

986.4812738

471.945355

c ψSi

20.26171875

37.73795535

32.87410926

a θLT (1)

0

0

0

c θLT

0

0

0

d TLTTS

0

0

0

d TLTTN

0

0

0

d TLTψSi

0

0

0

d TSTN

0

0

1862.994192

d TNψSi

0

0

0

d TNθLT

0

0

0

d TEψSi

0

0

0

d ψSiθLT

0

0

0

e

5317.859375

5103.813161

4853.204861

TABLE 5

s = 2,

Second

Higher-

Order

Mode

Si(100)

Si(110)

Si(111)

a TLT (2)

0

0

0

a TLT (1)

−608.2898721

−1003.471473

−1270.018362

b TLT (2)

0

0

0

c TLT

0.25

0.253954306

0.249121666

a TS (2)

0

0

0

a TS (1)

−1140.654415

−1030.75867

−1039.830158

b TS (2)

0

0

0

c TS

0.249966079

0.255272408

0.250032531

a TN (3)

−3219.596725

0

2822.963403

a TN (2)

555.8662451

0

−264.9680504

a TN (1)

465.8636149

53.04201209

−288.9461645

b TN (3)

0.001081155

0

0.000392787

b TN (2)

0.04654949

0

0.48934743

c TN

0.378426052

0.376449912

0.392908263

a TE (1)

0

−622.7635558

−614.5885324

c TE

0

0.151274165

0.156815224

a ψSi (4)

0

−0.00096736

−0.000227305

a ψSi (3)

0

−0.006772454

−0.00220017

a ψSi (2)

0

2.203099663

0.31727324

a ψSi (1)

0.833288758

28.15768206

0.648998523

b ψSi (4)

0

2959964.533

396965.3474

b ψSi (3)

0

19143.61126

87.44425969

b ψSi (2)

0

1447.367657

532.0008856

c ψSi

22.51017639

40.50966608

29.90240729

a θLT (1)

−1.501270796

−2.076046604

−2.376979261

c θLT

−52.08683853

−50.82249561

−49.04879636

d TLTTS

0

0

0

d TLTTN

0

0

0

d TLTψSi

0

16.61849238

0

d TSTN

0

1820.795615

1482.11565

d TNψSi

0

3.625908485

−3.131543418

d TNθLT

0

0

1607.412093

d TEψSi

0

0

0

d ψSiθLT

0

0

0.089566113

e

5326.187246

5356.110093

5418.323508

TABLE 6

s = 3,

Third

Higher-

Order

Mode

Si(100)

Si(110)

Si(111)

a TLT (2)

−14710.45271

0

0

a TLT (1)

−764.4056124

−942.2882121

−582.1313356

b TLT (2)

0.001558682

0

0

c TLT

0.257243963

0.255679719

0.251712062

a TS (2)

−21048.18754

0

0

a TS (1)

−508.6730943

−705.5211128

−400.0368899

b TS (2)

0.001583662

0

0

c TS

0.257243963

0.254751848

0.254357977

a TN (3)

0

0

0

a TN (2)

0

0

0

a TN (1)

0

97.59462013

24.94240828

b TN (3)

0

0

0

b TN (2)

0

0

0

c TN

0

0.367793031

0.404280156

a TE (1)

−276.7311066

−747.0884117

0

c TE

0.1494796

0.152164731

0

a ψSi (4)

0

0

−0.00075146

a ψSi (3)

0.011363183

0.003532214

−0.002666357

a ψSi (2)

−0.23320473

0.218669312

1.006728665

a ψSi (1)

0.214067146

−11.24365221

0.523191515

b ψSi (4)

0

0

381500.5075

b ψSi (3)

180.0564368

20914.04622

−493.6094588

b ψSi (2)

257.0498426

1548.182277

530.6814032

c ψSi

22.31890092

39.72544879

30.82490272

a θLT (1)

0

0

−1.551626054

c θLT

0

0

−49.16731518

d TLTTS

−13796.64706

0

1575.283126

d TLTTN

0

0

0

d TLTψSi

30.35701585

0

0

d TSTN

0

0

0

d TNψSi

0

0

0

d TNθLT

0

0

0

d TEψSi

28.27908094

0

0

d ψSiθLT

0

0

−0.086544362

e

5700.075407

5563.854277

5688.418884.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Feb 6, 2020
From: NAKAGAWA, RYO; NAGATOMO, SHOU; IWAMOTO, HIDEKI; TAKAI, TSUTOMU
To: MURATA MANUFACTURING CO., LTD.
Reel/Frame 051736/0087 →
Priority Claims (1)
JP JP2017-154239 · Aug 9, 2017 · national
Continuity (2)
Continuation PCTJP2018027358 · Jul 20, 2018
Related Publication 20200177157A1 · Jun 4, 2020
Cited By (1)
US 12,224,733