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 |
|---|---|---|---|---|---|---|---|---|---|
| 3047 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}X_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{3}M_{5}$ + ${ }M_{4}^{2}$ + ${ }M_{6}q_{2}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}^{2}$ | 0.565 | 0.7052 | 0.8012 | [X:[1.429], M:[0.9142, 0.571, 1.0858, 1.0, 0.9142, 0.7426, 1.1716], q:[0.8358, 0.75], qb:[0.25, 0.5074], phi:[0.4142]] | [X:[[5]], M:[[-1], [-5], [1], [0], [-1], [-3], [2]], q:[[1], [0]], qb:[[0], [3]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }M_{5}$, ${ }M_{4}$, ${ }M_{7}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{6}^{2}$, ${ }M_{6}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }q_{1}q_{2}$, ${ }M_{1}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{6}M_{7}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{7}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$ | ${}$ | -2 | t^2.228 + t^2.272 + 2*t^2.743 + t^3. + 2*t^3.515 + t^4.03 + t^4.287 + t^4.456 + t^4.5 + t^4.544 + t^4.757 + 2*t^4.97 + 2*t^5.015 + t^5.272 + 2*t^5.485 + 3*t^5.743 + 2*t^5.787 - 2*t^6. + 3*t^6.257 + t^6.302 - t^6.47 + t^6.515 + t^6.559 + t^6.684 + t^6.772 + t^6.816 + 4*t^7.03 + 2*t^7.198 + 2*t^7.287 + 2*t^7.544 + 2*t^7.713 + t^7.757 + t^7.802 + t^7.97 + t^8.015 + 3*t^8.059 - t^8.228 - 2*t^8.272 + t^8.316 + 4*t^8.485 + 2*t^8.53 + 2*t^8.574 - t^8.698 - 5*t^8.743 + t^8.787 + t^8.831 + t^8.911 + t^8.956 - t^4.243/y - t^6.47/y - t^6.985/y + (2*t^7.5)/y + (2*t^7.97)/y + (3*t^8.015)/y + t^8.228/y + t^8.272/y + t^8.485/y - t^8.698/y + (4*t^8.743)/y + (2*t^8.787)/y - t^4.243*y - t^6.47*y - t^6.985*y + 2*t^7.5*y + 2*t^7.97*y + 3*t^8.015*y + t^8.228*y + t^8.272*y + t^8.485*y - t^8.698*y + 4*t^8.743*y + 2*t^8.787*y | t^2.228/g1^3 + g1^3*t^2.272 + (2*t^2.743)/g1 + t^3. + 2*g1^2*t^3.515 + g1^4*t^4.03 + g1^5*t^4.287 + t^4.456/g1^6 + t^4.5 + g1^6*t^4.544 + g1*t^4.757 + (2*t^4.97)/g1^4 + 2*g1^2*t^5.015 + g1^3*t^5.272 + (2*t^5.485)/g1^2 + (3*t^5.743)/g1 + 2*g1^5*t^5.787 - 2*t^6. + 3*g1*t^6.257 + g1^7*t^6.302 - t^6.47/g1^4 + g1^2*t^6.515 + g1^8*t^6.559 + t^6.684/g1^9 + g1^3*t^6.772 + g1^9*t^6.816 + 4*g1^4*t^7.03 + (2*t^7.198)/g1^7 + 2*g1^5*t^7.287 + 2*g1^6*t^7.544 + (2*t^7.713)/g1^5 + g1*t^7.757 + g1^7*t^7.802 + t^7.97/g1^4 + g1^2*t^8.015 + 3*g1^8*t^8.059 - t^8.228/g1^3 - 2*g1^3*t^8.272 + g1^9*t^8.316 + (4*t^8.485)/g1^2 + 2*g1^4*t^8.53 + 2*g1^10*t^8.574 - t^8.698/g1^7 - (5*t^8.743)/g1 + g1^5*t^8.787 + g1^11*t^8.831 + t^8.911/g1^12 + t^8.956/g1^6 - t^4.243/(g1*y) - t^6.47/(g1^4*y) - t^6.985/(g1^2*y) + (2*t^7.5)/y + (2*t^7.97)/(g1^4*y) + (3*g1^2*t^8.015)/y + t^8.228/(g1^3*y) + (g1^3*t^8.272)/y + t^8.485/(g1^2*y) - t^8.698/(g1^7*y) + (4*t^8.743)/(g1*y) + (2*g1^5*t^8.787)/y - (t^4.243*y)/g1 - (t^6.47*y)/g1^4 - (t^6.985*y)/g1^2 + 2*t^7.5*y + (2*t^7.97*y)/g1^4 + 3*g1^2*t^8.015*y + (t^8.228*y)/g1^3 + g1^3*t^8.272*y + (t^8.485*y)/g1^2 - (t^8.698*y)/g1^7 + (4*t^8.743*y)/g1 + 2*g1^5*t^8.787*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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 1997 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}X_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{3}M_{5}$ + ${ }M_{4}^{2}$ + ${ }M_{6}q_{2}\tilde{q}_{2}$ | 0.5801 | 0.7306 | 0.794 | [X:[1.4597], M:[0.9081, 0.5403, 1.0919, 1.0, 0.9081, 0.7242], q:[0.8419, 0.75], qb:[0.25, 0.5258], phi:[0.4081]] | t^2.173 + t^2.327 + t^2.448 + 2*t^2.724 + t^3. + t^3.552 + t^4.103 + t^4.345 + t^4.379 + t^4.5 + t^4.621 + t^4.655 + 2*t^4.776 + 3*t^4.897 + 2*t^5.052 + 2*t^5.173 + t^5.327 + 3*t^5.448 + 2*t^5.724 + t^5.879 - t^6. - t^4.224/y - t^4.224*y | detail |