Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
# | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
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6066 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}M_{8}$ + ${ }M_{1}M_{7}$ + ${ }M_{6}X_{1}$ + ${ }M_{7}M_{9}$ | 0.5779 | 0.7326 | 0.7888 | [X:[1.3805], M:[1.0958, 0.8093, 1.1907, 0.7144, 1.2856, 0.6195, 0.9042, 0.8093, 1.0958], q:[0.4995, 0.4047], qb:[0.3098, 0.8809], phi:[0.4763]] | [X:[[22]], M:[[-26], [10], [-10], [-6], [6], [-22], [26], [10], [-26]], q:[[21], [5]], qb:[[-11], [1]], phi:[[-4]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{4}$, ${ }M_{2}$, ${ }M_{8}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{9}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{5}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}M_{8}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{8}$, ${ }M_{8}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}M_{9}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}M_{8}$, ${ }M_{2}M_{9}$, ${ }M_{8}M_{9}$, ${ }\phi_{1}^{4}$, ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$ | ${}M_{4}\phi_{1}q_{2}^{2}$, ${ }M_{4}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{8}\phi_{1}q_{2}\tilde{q}_{1}$ | -1 | t^2.143 + 2*t^2.428 + t^2.858 + 2*t^3.287 + t^3.572 + 3*t^3.857 + 2*t^4.141 + t^4.426 + t^4.571 + 2*t^4.856 + 2*t^5.001 + 3*t^5.286 + t^5.431 + t^5.57 + 3*t^5.715 - t^6. + 2*t^6.145 + 3*t^6.285 + 3*t^6.569 + 3*t^6.575 + 3*t^6.714 + 2*t^6.854 + t^6.86 + t^6.999 + 3*t^7.144 + 2*t^7.284 + 4*t^7.429 - t^7.568 - t^7.574 + 7*t^7.713 + t^7.859 + 5*t^7.998 - t^8.143 + 4*t^8.283 + 3*t^8.288 - 7*t^8.428 + 2*t^8.567 + 3*t^8.573 - 2*t^8.713 + t^8.718 + t^8.852 + 2*t^8.997 - t^4.429/y - t^6.857/y + t^7.141/y - t^7.287/y + (3*t^7.571)/y - t^7.716/y + t^7.856/y + (2*t^8.001)/y + (2*t^8.286)/y + (2*t^8.431)/y + (5*t^8.715)/y - t^4.429*y - t^6.857*y + t^7.141*y - t^7.287*y + 3*t^7.571*y - t^7.716*y + t^7.856*y + 2*t^8.001*y + 2*t^8.286*y + 2*t^8.431*y + 5*t^8.715*y | t^2.143/g1^6 + 2*g1^10*t^2.428 + t^2.858/g1^8 + (2*t^3.287)/g1^26 + t^3.572/g1^10 + 3*g1^6*t^3.857 + 2*g1^22*t^4.141 + g1^38*t^4.426 + g1^4*t^4.571 + 2*g1^20*t^4.856 + (2*t^5.001)/g1^14 + 3*g1^2*t^5.286 + t^5.431/g1^32 + g1^18*t^5.57 + (3*t^5.715)/g1^16 - t^6. + (2*t^6.145)/g1^34 + 3*g1^16*t^6.285 + 3*g1^32*t^6.569 + (3*t^6.575)/g1^52 + (3*t^6.714)/g1^2 + 2*g1^48*t^6.854 + t^6.86/g1^36 + g1^14*t^6.999 + (3*t^7.144)/g1^20 + 2*g1^30*t^7.284 + (4*t^7.429)/g1^4 - g1^46*t^7.568 - t^7.574/g1^38 + 7*g1^12*t^7.713 + t^7.859/g1^22 + 5*g1^28*t^7.998 - t^8.143/g1^6 + 4*g1^44*t^8.283 + (3*t^8.288)/g1^40 - 7*g1^10*t^8.428 + 2*g1^60*t^8.567 + (3*t^8.573)/g1^24 - 2*g1^26*t^8.713 + t^8.718/g1^58 + g1^76*t^8.852 + 2*g1^42*t^8.997 - t^4.429/(g1^4*y) - (g1^6*t^6.857)/y + (g1^22*t^7.141)/y - t^7.287/(g1^12*y) + (3*g1^4*t^7.571)/y - t^7.716/(g1^30*y) + (g1^20*t^7.856)/y + (2*t^8.001)/(g1^14*y) + (2*g1^2*t^8.286)/y + (2*t^8.431)/(g1^32*y) + (5*t^8.715)/(g1^16*y) - (t^4.429*y)/g1^4 - g1^6*t^6.857*y + g1^22*t^7.141*y - (t^7.287*y)/g1^12 + 3*g1^4*t^7.571*y - (t^7.716*y)/g1^30 + g1^20*t^7.856*y + (2*t^8.001*y)/g1^14 + 2*g1^2*t^8.286*y + (2*t^8.431*y)/g1^32 + (5*t^8.715*y)/g1^16 |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
# | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
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Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|---|
4566 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}M_{8}$ + ${ }M_{1}M_{7}$ + ${ }M_{6}X_{1}$ | 0.5887 | 0.7531 | 0.7818 | [X:[1.3387], M:[1.1451, 0.7903, 1.2097, 0.7258, 1.2742, 0.6613, 0.8549, 0.7903], q:[0.4597, 0.3952], qb:[0.3306, 0.879], phi:[0.4839]] | t^2.177 + 2*t^2.371 + t^2.565 + t^2.903 + t^3.435 + t^3.629 + 3*t^3.823 + 2*t^4.016 + t^4.21 + t^4.548 + 3*t^4.742 + 2*t^4.936 + 2*t^5.081 + t^5.129 + 3*t^5.274 + 2*t^5.468 + t^5.806 - t^4.452/y - t^4.452*y | detail |