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 |
|---|---|---|---|---|---|---|---|---|---|
| 48253 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{5}^{2}$ | 0.696 | 0.8516 | 0.8172 | [M:[0.9617, 1.0191, 1.0383, 0.9426, 1.0], q:[0.4713, 0.567], qb:[0.5096, 0.4904], phi:[0.4904]] | [M:[[4], [-2], [-4], [6], [0]], q:[[3], [-7]], qb:[[-1], [1]], phi:[[1]]] |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }M_{2}$, ${ }M_{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{1}M_{5}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{2}$, ${ }M_{3}M_{4}$, ${ }M_{5}\phi_{1}^{2}$ | ${}$ | -1 | t^2.828 + t^2.885 + t^2.943 + t^3. + t^3.057 + t^3.115 + t^3.23 + t^4.299 + t^4.356 + 2*t^4.414 + t^4.471 + t^4.529 + t^4.586 + t^4.644 + t^4.701 + t^4.873 + t^5.655 + t^5.77 + t^5.828 + 2*t^5.885 + t^5.943 - t^6. + t^6.057 + t^6.115 + t^6.172 + t^6.23 + t^6.345 + t^6.46 + t^7.127 + t^7.184 + 3*t^7.242 + 3*t^7.299 + 3*t^7.356 + 3*t^7.414 + t^7.471 + 3*t^7.529 + t^7.586 + 2*t^7.644 + 2*t^7.701 + t^7.758 + 2*t^7.816 + t^7.873 + t^7.931 + t^7.988 + t^8.103 + t^8.483 + 2*t^8.598 + t^8.655 + 3*t^8.713 + 2*t^8.77 + t^8.885 - t^8.943 - t^4.471/y - t^7.299/y + t^7.644/y + t^8.713/y + t^8.77/y + (2*t^8.828)/y + (2*t^8.885)/y + (3*t^8.943)/y - t^4.471*y - t^7.299*y + t^7.644*y + t^8.713*y + t^8.77*y + 2*t^8.828*y + 2*t^8.885*y + 3*t^8.943*y | g1^6*t^2.828 + g1^4*t^2.885 + g1^2*t^2.943 + t^3. + t^3.057/g1^2 + t^3.115/g1^4 + t^3.23/g1^8 + g1^7*t^4.299 + g1^5*t^4.356 + 2*g1^3*t^4.414 + g1*t^4.471 + t^4.529/g1 + t^4.586/g1^3 + t^4.644/g1^5 + t^4.701/g1^7 + t^4.873/g1^13 + g1^12*t^5.655 + g1^8*t^5.77 + g1^6*t^5.828 + 2*g1^4*t^5.885 + g1^2*t^5.943 - t^6. + t^6.057/g1^2 + t^6.115/g1^4 + t^6.172/g1^6 + t^6.23/g1^8 + t^6.345/g1^12 + t^6.46/g1^16 + g1^13*t^7.127 + g1^11*t^7.184 + 3*g1^9*t^7.242 + 3*g1^7*t^7.299 + 3*g1^5*t^7.356 + 3*g1^3*t^7.414 + g1*t^7.471 + (3*t^7.529)/g1 + t^7.586/g1^3 + (2*t^7.644)/g1^5 + (2*t^7.701)/g1^7 + t^7.758/g1^9 + (2*t^7.816)/g1^11 + t^7.873/g1^13 + t^7.931/g1^15 + t^7.988/g1^17 + t^8.103/g1^21 + g1^18*t^8.483 + 2*g1^14*t^8.598 + g1^12*t^8.655 + 3*g1^10*t^8.713 + 2*g1^8*t^8.77 + g1^4*t^8.885 - g1^2*t^8.943 - (g1*t^4.471)/y - (g1^7*t^7.299)/y + t^7.644/(g1^5*y) + (g1^10*t^8.713)/y + (g1^8*t^8.77)/y + (2*g1^6*t^8.828)/y + (2*g1^4*t^8.885)/y + (3*g1^2*t^8.943)/y - g1*t^4.471*y - g1^7*t^7.299*y + (t^7.644*y)/g1^5 + g1^10*t^8.713*y + g1^8*t^8.77*y + 2*g1^6*t^8.828*y + 2*g1^4*t^8.885*y + 3*g1^2*t^8.943*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 |
|---|---|---|---|---|---|---|---|---|
| 55969 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{5}^{2}$ + ${ }M_{6}\phi_{1}^{2}$ | 0.6943 | 0.8492 | 0.8177 | [M:[0.9694, 1.0153, 1.0306, 0.9541, 1.0, 1.0153], q:[0.477, 0.5536], qb:[0.5077, 0.4923], phi:[0.4923]] | t^2.862 + t^2.908 + t^3. + 2*t^3.046 + t^3.092 + t^3.184 + t^4.339 + t^4.385 + 2*t^4.431 + t^4.477 + t^4.523 + t^4.569 + t^4.615 + t^4.661 + t^4.799 + t^5.724 + 2*t^5.908 + t^5.954 - 2*t^6. - t^4.477/y - t^4.477*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 |
|---|
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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 46383 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ | 0.7095 | 0.8721 | 0.8136 | [M:[1.0279, 1.0487, 0.9721, 0.8538, 0.8746], q:[0.4269, 0.5452], qb:[0.5244, 0.601], phi:[0.4756]] | t^2.561 + t^2.624 + t^2.854 + t^2.916 + t^3.084 + t^3.146 + t^3.209 + t^3.988 + t^4.281 + t^4.343 + t^4.511 + t^4.573 + t^4.636 + t^4.698 + t^4.803 + t^4.866 + t^5.033 + t^5.123 + t^5.185 + t^5.248 + t^5.415 + t^5.478 + t^5.54 + 2*t^5.708 + 2*t^5.77 + t^5.832 - 2*t^6. - t^4.427/y - t^4.427*y | detail |