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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56370 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ + ${ }M_{5}^{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{7}\phi_{1}q_{1}q_{2}$ + ${ }M_{2}X_{1}$ | 0.6051 | 0.7555 | 0.8009 | [X:[1.3339], M:[1.222, 0.6661, 0.778, 0.9633, 1.0, 0.8514, 0.8147], q:[0.4816, 0.2963], qb:[0.8522, 0.7404], phi:[0.4073]] | [X:[[18]], M:[[-6], [-18], [6], [10], [0], [-14], [-4]], q:[[5], [1]], qb:[[13], [-11]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{3}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{6}$, ${ }M_{4}$, ${ }M_{5}$, ${ }M_{1}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{3}M_{7}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{6}$, ${ }M_{7}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{6}M_{7}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{6}^{2}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{7}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{4}^{2}$ | ${}$ | -1 | t^2.334 + 2*t^2.444 + t^2.554 + t^2.89 + t^3. + t^3.666 + t^4.002 + t^4.112 + t^4.668 + 3*t^4.778 + 4*t^4.888 + 2*t^4.998 + t^5.109 + t^5.224 + 3*t^5.334 + 2*t^5.444 + t^5.78 - t^6. + t^6.11 + t^6.22 + t^6.335 + 2*t^6.446 + 2*t^6.556 - t^6.776 + t^6.891 + 2*t^7.002 + 3*t^7.222 + 7*t^7.332 + 4*t^7.442 + 2*t^7.553 + t^7.663 + 3*t^7.668 + 5*t^7.778 + 2*t^7.888 + t^8.003 + 2*t^8.113 + 2*t^8.224 - 3*t^8.334 - 4*t^8.444 - t^8.554 + t^8.665 + 2*t^8.669 + t^8.775 + 2*t^8.78 - t^4.222/y - (2*t^6.666)/y - t^6.776/y - t^7.112/y + t^7.332/y + t^7.668/y + (4*t^7.778)/y + (2*t^7.888)/y + (2*t^7.998)/y + t^8.224/y + (3*t^8.334)/y + (3*t^8.444)/y + t^8.554/y + t^8.89/y - t^4.222*y - 2*t^6.666*y - t^6.776*y - t^7.112*y + t^7.332*y + t^7.668*y + 4*t^7.778*y + 2*t^7.888*y + 2*t^7.998*y + t^8.224*y + 3*t^8.334*y + 3*t^8.444*y + t^8.554*y + t^8.89*y | g1^6*t^2.334 + (2*t^2.444)/g1^4 + t^2.554/g1^14 + g1^10*t^2.89 + t^3. + t^3.666/g1^6 + g1^18*t^4.002 + g1^8*t^4.112 + g1^12*t^4.668 + 3*g1^2*t^4.778 + (4*t^4.888)/g1^8 + (2*t^4.998)/g1^18 + t^5.109/g1^28 + g1^16*t^5.224 + 3*g1^6*t^5.334 + (2*t^5.444)/g1^4 + g1^20*t^5.78 - t^6. + t^6.11/g1^10 + t^6.22/g1^20 + g1^24*t^6.335 + 2*g1^14*t^6.446 + 2*g1^4*t^6.556 - t^6.776/g1^16 + g1^28*t^6.891 + 2*g1^18*t^7.002 + (3*t^7.222)/g1^2 + (7*t^7.332)/g1^12 + (4*t^7.442)/g1^22 + (2*t^7.553)/g1^32 + t^7.663/g1^42 + 3*g1^12*t^7.668 + 5*g1^2*t^7.778 + (2*t^7.888)/g1^8 + g1^36*t^8.003 + 2*g1^26*t^8.113 + 2*g1^16*t^8.224 - 3*g1^6*t^8.334 - (4*t^8.444)/g1^4 - t^8.554/g1^14 + t^8.665/g1^24 + 2*g1^30*t^8.669 + t^8.775/g1^34 + 2*g1^20*t^8.78 - t^4.222/(g1^2*y) - (2*t^6.666)/(g1^6*y) - t^6.776/(g1^16*y) - (g1^8*t^7.112)/y + t^7.332/(g1^12*y) + (g1^12*t^7.668)/y + (4*g1^2*t^7.778)/y + (2*t^7.888)/(g1^8*y) + (2*t^7.998)/(g1^18*y) + (g1^16*t^8.224)/y + (3*g1^6*t^8.334)/y + (3*t^8.444)/(g1^4*y) + t^8.554/(g1^14*y) + (g1^10*t^8.89)/y - (t^4.222*y)/g1^2 - (2*t^6.666*y)/g1^6 - (t^6.776*y)/g1^16 - g1^8*t^7.112*y + (t^7.332*y)/g1^12 + g1^12*t^7.668*y + 4*g1^2*t^7.778*y + (2*t^7.888*y)/g1^8 + (2*t^7.998*y)/g1^18 + g1^16*t^8.224*y + 3*g1^6*t^8.334*y + (3*t^8.444*y)/g1^4 + (t^8.554*y)/g1^14 + g1^10*t^8.89*y |
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 |
---|---|---|---|---|---|---|---|---|---|
51892 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ + ${ }M_{5}^{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ | 0.6104 | 0.7697 | 0.793 | [M:[1.2253, 0.676, 0.7747, 0.9578, 1.0, 0.8591], q:[0.4789, 0.2958], qb:[0.8451, 0.7464], phi:[0.4084]] | t^2.028 + t^2.324 + t^2.451 + t^2.577 + t^2.873 + t^3. + t^3.549 + t^3.676 + t^4.056 + t^4.099 + t^4.352 + t^4.479 + t^4.605 + t^4.648 + 2*t^4.775 + 3*t^4.901 + 2*t^5.028 + t^5.155 + t^5.197 + 2*t^5.324 + t^5.451 + t^5.577 + t^5.704 + t^5.747 + t^5.873 - t^4.225/y - t^4.225*y | detail |