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 |
---|---|---|---|---|---|---|---|---|---|
46194 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}^{4}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | 0.6728 | 0.8725 | 0.7711 | [M:[1.1331, 0.696, 0.804, 0.6709], q:[0.75, 0.4209], qb:[0.3831, 0.446], phi:[0.5]] | [M:[[1, 0], [0, 1], [0, -1], [-1, -1]], q:[[0, 0], [-1, -1]], qb:[[1, 0], [0, 1]], phi:[[0, 0]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{4}$, ${ }M_{2}$, ${ }M_{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{2}M_{3}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{2}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}q_{1}q_{2}$, ${ }M_{2}q_{1}q_{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}q_{1}\tilde{q}_{1}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }M_{2}\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{3}q_{1}q_{2}$, ${ }q_{1}q_{2}^{2}\tilde{q}_{1}$ | ${}$ | -2 | t^2.013 + t^2.088 + 2*t^2.412 + t^2.487 + t^3. + 2*t^3.399 + t^3.513 + t^3.798 + 2*t^4.026 + 2*t^4.101 + 2*t^4.176 + 2*t^4.425 + 3*t^4.5 + t^4.575 + 3*t^4.824 + 2*t^4.899 + t^4.974 + t^5.013 + t^5.088 + 4*t^5.412 + 3*t^5.487 + t^5.526 + t^5.601 + 4*t^5.811 + 2*t^5.886 + t^5.925 - 2*t^6. + 2*t^6.038 - t^6.075 + 2*t^6.114 + 2*t^6.189 + 2*t^6.21 + 2*t^6.264 + t^6.286 + 4*t^6.438 + 5*t^6.513 + 4*t^6.588 + 2*t^6.663 + 3*t^6.798 + 3*t^6.837 + 5*t^6.912 + t^6.987 + 2*t^7.026 + t^7.062 + t^7.176 + 2*t^7.198 + 4*t^7.236 + 2*t^7.311 + 4*t^7.425 + t^7.462 + 3*t^7.5 + 2*t^7.538 + 3*t^7.575 + t^7.597 + 7*t^7.824 + 6*t^7.899 + t^7.938 + 3*t^7.974 - 3*t^8.013 + 3*t^8.051 - 5*t^8.088 + 3*t^8.126 - t^8.163 + 3*t^8.202 + 6*t^8.223 + 3*t^8.277 + 4*t^8.298 + t^8.337 + 3*t^8.352 + 2*t^8.374 - 5*t^8.412 + 4*t^8.45 - 4*t^8.487 + 5*t^8.526 - t^8.562 + 3*t^8.601 + 3*t^8.622 + 4*t^8.676 + 2*t^8.698 + 2*t^8.751 + t^8.773 + 2*t^8.811 + 6*t^8.85 + 2*t^8.886 + 7*t^8.925 - t^4.5/y - t^6.513/y - t^6.588/y - t^6.912/y + (2*t^7.101)/y + (2*t^7.425)/y + (3*t^7.5)/y + t^7.575/y + t^7.824/y + t^7.899/y + t^8.013/y + (2*t^8.088)/y + (5*t^8.412)/y + (4*t^8.487)/y - t^8.676/y + (5*t^8.811)/y + (3*t^8.886)/y + t^8.925/y - t^4.5*y - t^6.513*y - t^6.588*y - t^6.912*y + 2*t^7.101*y + 2*t^7.425*y + 3*t^7.5*y + t^7.575*y + t^7.824*y + t^7.899*y + t^8.013*y + 2*t^8.088*y + 5*t^8.412*y + 4*t^8.487*y - t^8.676*y + 5*t^8.811*y + 3*t^8.886*y + t^8.925*y | t^2.013/(g1*g2) + g2*t^2.088 + (2*t^2.412)/g2 + g1*g2*t^2.487 + t^3. + 2*g1*t^3.399 + t^3.513/(g1*g2) + g1^2*t^3.798 + (2*t^4.026)/(g1^2*g2^2) + (2*t^4.101)/g1 + 2*g2^2*t^4.176 + (2*t^4.425)/(g1*g2^2) + 3*t^4.5 + g1*g2^2*t^4.575 + (3*t^4.824)/g2^2 + 2*g1*t^4.899 + g1^2*g2^2*t^4.974 + t^5.013/(g1*g2) + g2*t^5.088 + (4*t^5.412)/g2 + 3*g1*g2*t^5.487 + t^5.526/(g1^2*g2^2) + t^5.601/g1 + (4*g1*t^5.811)/g2 + 2*g1^2*g2*t^5.886 + t^5.925/(g1*g2^2) - 2*t^6. + (2*t^6.038)/(g1^3*g2^3) - g1*g2^2*t^6.075 + (2*t^6.114)/(g1^2*g2) + (2*g2*t^6.189)/g1 + (2*g1^2*t^6.21)/g2 + 2*g2^3*t^6.264 + g1^3*g2*t^6.286 + (4*t^6.438)/(g1^2*g2^3) + (5*t^6.513)/(g1*g2) + 4*g2*t^6.588 + 2*g1*g2^3*t^6.663 + 3*g1^2*t^6.798 + (3*t^6.837)/(g1*g2^3) + (5*t^6.912)/g2 + g1*g2*t^6.987 + (2*t^7.026)/(g1^2*g2^2) + g1^2*g2^3*t^7.062 + g2^2*t^7.176 + 2*g1^3*t^7.198 + (4*t^7.236)/g2^3 + (2*g1*t^7.311)/g2 + (4*t^7.425)/(g1*g2^2) + g1^3*g2^3*t^7.462 + 3*t^7.5 + (2*t^7.538)/(g1^3*g2^3) + 3*g1*g2^2*t^7.575 + g1^4*t^7.597 + (7*t^7.824)/g2^2 + 6*g1*t^7.899 + t^7.938/(g1^2*g2^3) + 3*g1^2*g2^2*t^7.974 - (3*t^8.013)/(g1*g2) + (3*t^8.051)/(g1^4*g2^4) - 5*g2*t^8.088 + (3*t^8.126)/(g1^3*g2^2) - g1*g2^3*t^8.163 + (3*t^8.202)/g1^2 + (6*g1*t^8.223)/g2^2 + (3*g2^2*t^8.277)/g1 + 4*g1^2*t^8.298 + t^8.337/(g1*g2^3) + 3*g2^4*t^8.352 + 2*g1^3*g2^2*t^8.374 - (5*t^8.412)/g2 + (4*t^8.45)/(g1^3*g2^4) - 4*g1*g2*t^8.487 + (5*t^8.526)/(g1^2*g2^2) - g1^2*g2^3*t^8.562 + (3*t^8.601)/g1 + (3*g1^2*t^8.622)/g2^2 + 4*g2^2*t^8.676 + 2*g1^3*t^8.698 + 2*g1*g2^4*t^8.751 + g1^4*g2^2*t^8.773 + (2*g1*t^8.811)/g2 + (6*t^8.85)/(g1^2*g2^4) + 2*g1^2*g2*t^8.886 + (7*t^8.925)/(g1*g2^2) - t^4.5/y - t^6.513/(g1*g2*y) - (g2*t^6.588)/y - t^6.912/(g2*y) + (2*t^7.101)/(g1*y) + (2*t^7.425)/(g1*g2^2*y) + (3*t^7.5)/y + (g1*g2^2*t^7.575)/y + t^7.824/(g2^2*y) + (g1*t^7.899)/y + t^8.013/(g1*g2*y) + (2*g2*t^8.088)/y + (5*t^8.412)/(g2*y) + (4*g1*g2*t^8.487)/y - (g2^2*t^8.676)/y + (5*g1*t^8.811)/(g2*y) + (3*g1^2*g2*t^8.886)/y + t^8.925/(g1*g2^2*y) - t^4.5*y - (t^6.513*y)/(g1*g2) - g2*t^6.588*y - (t^6.912*y)/g2 + (2*t^7.101*y)/g1 + (2*t^7.425*y)/(g1*g2^2) + 3*t^7.5*y + g1*g2^2*t^7.575*y + (t^7.824*y)/g2^2 + g1*t^7.899*y + (t^8.013*y)/(g1*g2) + 2*g2*t^8.088*y + (5*t^8.412*y)/g2 + 4*g1*g2*t^8.487*y - g2^2*t^8.676*y + (5*g1*t^8.811*y)/g2 + 3*g1^2*g2*t^8.886*y + (t^8.925*y)/(g1*g2^2) |
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 |
---|---|---|---|---|---|---|---|---|
46703 | ${}\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}^{4}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{5}q_{1}q_{2}$ | 0.688 | 0.8991 | 0.7652 | [M:[1.1225, 0.6887, 0.8113, 0.6887, 0.8113], q:[0.75, 0.4387], qb:[0.3725, 0.4387], phi:[0.5]] | 2*t^2.066 + 4*t^2.434 + t^3. + 2*t^3.368 + t^3.735 + 6*t^4.132 + 8*t^4.5 + 10*t^4.868 + 2*t^5.066 + 8*t^5.434 + 8*t^5.801 - 5*t^6. - t^4.5/y - t^4.5*y | detail | |
46425 | ${}\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}^{4}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }q_{1}q_{2}^{2}\tilde{q}_{1}$ | 0.6724 | 0.8714 | 0.7716 | [M:[1.1326, 0.6837, 0.8163, 0.6837], q:[0.75, 0.4337], qb:[0.3826, 0.4337], phi:[0.5]] | 2*t^2.051 + 3*t^2.449 + t^3. + 2*t^3.398 + t^3.551 + t^3.795 + 6*t^4.102 + 6*t^4.5 + 6*t^4.898 + 2*t^5.051 + 7*t^5.449 + 2*t^5.602 + 6*t^5.846 - 2*t^6. - t^4.5/y - t^4.5*y | detail |
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 |
---|---|---|---|---|---|---|---|---|---|
46052 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}^{4}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ | 0.652 | 0.8312 | 0.7844 | [M:[1.1326, 0.6957, 0.8043], q:[0.75, 0.4217], qb:[0.3826, 0.4457], phi:[0.5]] | t^2.087 + 2*t^2.413 + t^2.485 + t^3. + 2*t^3.398 + t^3.515 + t^3.796 + t^3.985 + t^4.03 + t^4.102 + 2*t^4.174 + 2*t^4.5 + t^4.572 + 3*t^4.826 + 2*t^4.898 + t^4.97 + t^5.087 + 2*t^5.413 + 3*t^5.485 + t^5.602 + 3*t^5.811 + 2*t^5.883 + t^5.928 - 2*t^6. - t^4.5/y - t^4.5*y | detail |